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THE SCIENTIFIC DISCOVERIES OF
PROF. RUGGERO MARIA SANTILLI
Prepared by the Board of Directors of the Foundation
following Prof. Santilli's guidelines and quoptations
Preliminary and partial draft
dated October 18, 2008
for comments please contact
"board(at)santilli-foundation(dot)org"
TABLE OF CONTENT
PREFACE
1. INSUFFICIENCIES OF THE 20-TH CENTURY THEORIES
1.1. THE LEGACY OF LAGRANGE AND HAMILTON.
1.2. INSUFFICIENCIES OF SPECIAL RELATIVITY
1.3. INSUFFICIENCIES OF GENERAL RELATIVITY
1.4. INSUFFICIENCIES OF EINSTEIN'S THEORIES FOR ANTIMATTER
1.5. INSUFFICIENCIES OF QUANTUM MECHANICS
1.6. INSUFFICIENCIES OF NUCLEAR PHYSICS
1.7. INSUFFICIENCIES OF PARTICLE PHYSICS
1.8. INSUFFICIENCIES OF QUARKS AND NEUTRINOS CONJECTURES
1.9. INSUFFICIENCIES OF QUANTUM CHEMISTRY
1.10. INSUFFICIENCIES OF BIOLOGY
1.11. INSUFFICIENCIES OF ASTROPHYSICS AND COSMOLOGY
1.12. INTRODUCTORY READINGS
2. SANTILLI'S DISCOVERIES IN MATHEMATICS
2.1. FOREWORD
2.2. DISCOVERY OF NEW NUMBERS
2.2A. Discovery of isonumbers (1983)
2.2B. Discovery of genonumbers (1993)
2.2C. Discovery of hypernumbers (1994)
2.2D. Discovery of isodual numbers (1993)
2.3. ISO-, DISCOVERY OF GENO-, HYPER-DIFFERENTIAL CALCULI AND THEIR ISODUALS (1996)
2.4. DISCOVERY OF ISO-, GENO-, HYPER-, SPACES AND THEIR ISODUALS (1983).
2.5. DISCOVERY OF ISO-, GENO-, HYPER-SYMPLECTIC GEOMETRIES AND THEIR ISODUALS (1996)
2.6. UNIFICATION OF MINKOWSKIAN AND RIEMANNIAN GEOMETRIES (1998)
2.7. ISOTOPIC COVERING OF LIE'S THEORY AND ITS ISODUAL (1978)
2.8. LIE-ADMISSIBLE COVERING OF THE LIE-ISOTOPIC THEORY AND ITS ISODUAL (1967)
2.9. INTEGRABILITY CONDITIONS FOR THE EXISTENCE OF A LAGRANGIAN
2.9A. Integrability conditions in Newtonian mechanics (1978).
2.9B. Integrability conditions in field theory (1975)
3. SANTILLI'S DISCOVERIES IN PHYSICS
3.1. FOREWORD
3.2. ETHER AS A UNIVERSAL SUBSTRATUM (1952-1955)
3.3. ORIGIN OF THE ELECTRIC AND MAGNETIC FIELDS (1955-1957)
Ethical notes
3.4. ORIGIN OF THE GRAVITATIONAL FIELD (1974)
Ethical notes
3.5. SYMMETRY OF THE ETHER (1970)
Ethical notes
3.6. QFT (AND QCD) LIMITS FROM DISCRETE SYMMETRY VIOLATIONS (1974)
Ethical notes
3.7. RESOLUTION OF THE HISTORICAL IMBALANCE ON ANTIMATTER (1994)
3.7A. Newton-Santilli isodual equation for antimatter
3.7B. Isodual representation of the Coulomb force
3.7C. Hamilton-Santilli isodual mechanics
3.7D. Isodual special and general relativities
3.7E. Antigravity
3.7F. Experiment on antigravity
3.7G. Isodual quantum mechanics
3.7H. Experimental detection of antimatter galaxies
3.7I. The new isoselfdual invariance of Dirac's equation
3.7J. Isoselfdual spacetime machine
3.7K. Original literature
Ethical notes
3.8. INITIATION OF q-DEFORMATIONS OF LIE THEORY
Ethical notes
3.9. THEOREMS OF CATASTROPHIC INCONSISTENCIES OF
NONCANONICAL AND NONUNITARY THEORIES
The majestic consistency of Hamiltonian theories.
3.9B. Theorems of catastrophic inconsistencies of noncanonical and nonunitary theories.
3.9C Examples of catastrophically inconsistent theories.
Ethical notes
3.10. SANTILLI ISO-, GENO-, AND HYPER-RELATIVITIES AND THEIR ISODUALS (1978)
3.10A. Historical notes
3.10B. Santilli's opening statement
3.10C. Coneceptual foundations
3.10D. Mathematical foundations
3.10E. Invariance and universality of Santilli's isotopies.
3.10F. Poincare'-Santilli isosymmetry and its isodual
3.10G. Isorelativity and its isodual
3.10H. Experimental verifications
3.10I. Isogravitation and its isodual
3.10J. Absence of expansion of the universe
3.10K. Absence of dark matter in the universe
3.10L. Proposed astrophysical experiments
3.10M. Isotopic reconstruction of exact spacetime symmetries when conventionally broken
3.10N. Geno- and hyper-relativities and their isoduals
3.10O. Primary literature
Ethical noltes
3.9. HADRONIC MECHANICS
UNDER CONSTRUCTION
<3,9A. Foreword
Newton-Santilli isoequations
Hamilton-0Santilli isomechanics
Animalu-Santilli isoquantization
Heoisenberg-Santilli isoequations
Experimemntal verifications
Primary literature
Ethical notes
NEUTRON SYNTHESIS
MESONS SYNTHESIS
KALNAY-SANTILLI QUARK CONFINEMENT
3. SANTILLI DISCOVERIES IN CHEMISTRY
3. EPILOGUE
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PREFACE
By using a language accessible to the general scientific audience, this web page is dedicated to an outline of the scientific discoveries by the Italian-American scientist Ruggero Maria Santilli ("Santilli" hereon) by providing a summary of the discoveries and making available the original contributions in free pdf downloads since they are at times of difficult location.
Santilli's discoveries have been the subject of a large number of contributions by scientists around the world we regret not to be able to review here to prevent a prohibitive length. For contributions by other authors, interested scholars may consult the 90 pages long
General Bibliography on Santilli Discoveries
Interested researchers or historians are suggested to exercise caution in using preprints of various works that are still circulating in the scientific community, because Santilli had the habit of quickly writing papers, sending them to colleagues for comments and criticisms, and finalizing them only at the time of publication. In same cases, due to the vast nature of the scientific production and Santilli's multiple duties, unedited versions ended up being published, thus requiring errata-corrige. Serious scholars should be aware of this occurrence, and verify the final character of the papers prior to expressing their views. In the event verifications of final character of a given work is needed, scholars are suggested to contact "board(at)santilli-foundation(dot)org".
1. INSUFFICIENCIES OF THE 20-TH CENTURY THEORIES
1.1. THE LEGACY OF LAGRANGE AND HAMILTON.
Santilli conducted his graduate studies in theoretical physics in the late 1960s at the University of Torino, Italy, where J. L. Lagrange lived and conducted his research. In this way, Santilli had the opportunity of studying the original papers by Lagrange (some of which had been written in Italian), thus learning Lagrange's originator conception of his celebrated analytic representation of nature (dating to 1788) as requiring two quantities:
1) A function L(r, v) = K(v) - V(r), today known as the Lagrangian, where r = (rk), k = 1, 2, 3, are the coordinates, v = dr/dt represents the velocity, K(v) = v2 m/2 is the kinetic energy, and V(r) represents all action-at-a-distance forces derivable from a potential, plus
2) The external terms, F(t, r, v), that is, terms external to his analytic equations representing all forces not derivable from a potential or a Lagrangian.
Santilli then studied in British libraries the original works by W. R. Hamilton and discovered that in 1834 he had essentially the same conception as that by Lagrange for the analytic representation of nature as characterized by a function, today known as the hamiltonian representing the total energy in a space (today called cotangent bundle) with local coordinates r and p = m v,
(1.1) H(r, p) = K(p) + V(r) = p2/2m + V(r),
plus his celebrated analytic equations, those with external terms representing forces non derivable from a potential (hereon called "non-Hamiltonian forces"),
(1.2) dr/dt = ∂H(r, p)/∂p, dp/dt = - ∂H(r, p)/∂r + F(t, r, p, ...).
The above analytic representation of nature remained in full force and effect until the early 1900. As an example, C. G. Jacobi formulated his celebrated theorem in 1837, not in the form presented in mechanics books of the 20-th century where the external terms are generally removed, but for the true Lagrange and Hamilton equations, those with external terms.
The advent in the early 1900 of special relativity and quantum mechanics caused a major alteration of the original analytic conception of nature by Lagrange and Hamilton. In essence, both special relativity and quantum mechanics are strictly Hamiltonian theories, that is, they only admit one quantity, a Lagrangian or, equivalently, a Hamiltonian, and show no possibility of accommodating the external terms short of a major structural revisions.
Consequently, the widespread posture of the 20-th century physics was to eliminate Lagrange and Hamilton external terms and solely work with equations today called the truncated Lagrange and Hamilton equations. A general argument was that the forces represented by the external terms are "fictitious" (sic) because, the argument says, when a system in our environment is reduced to its elementary constituents, all non-Lagrangian or non-Hamiltonian forces "disappear" (sic) and nature assumes the analytic structure of the truncated equations.
The first historical scientific contribution by Santilli was to formulate and prove the following theorem shopwing that the above posture is a mere manifestation of academic politics without scientific credibility.
\
THEOREM 1.1: A macroscopic system with forces that are nonconservative and/or irreversible over time cannot be consistently decomposed into a finite number of elementary particles all with solely conservative forces derivable from a potential and, vice versa, a finite number of elementary particles all in conservative conditions cannot consistently yield, under the correspondence principle or other means, a macroscopic system with nonconservative and/or irreversible forces.
The historical character of this theorem is set by the fact that the non-Lagrangian or non-Hamiltonian forces of our macroscopic environment, rather than "disappearing" at the particle level to please academia, originate at the most elementary level of nature, thus confirming the depth of the analytic conception of nature by Lagrange and Hamilton.
As an illustration, Theorem 1.1 establishes that the resistance experienced by a spaceship during re-enmtry in our atmosphere is due to the superposition of a large n umber of contact, nonlinear, nonlocal and nonpotential interactions between the peripheral atomicv electrons of the spaceship and corresponding atomic electrons in the atmosphere.
Another significance of Santilli's Theorem 1.1 is to establish ab initio that special relativity and quantum mechanics are not universal theories valid for all possible conditions in nature and for the rest of time, as essentially implied by a widespread posture of the 20-th century science, but have instead clear limitations.
Numerous additional historical implications of Theorem 1.1 will be indicated throughout this presentation. At this moment, we merely mention the huge technical difficulties caused by the inclusion of external terms in the analytic equations. In essence, the physics of the 20-th century was based on Lie algebras with antisymmetric brackets [A, B] = - [B, A] that appear in the time evolution of a physical quantity Q(r, p) of the truncated Hamilton's equations, dQ/dt = [Q, H], where the brackets are the celebrated Poisson brackets. The appearance of Lie algebras at the foundation of dynamics, the time evolution, then allowed a rigorous construction of the various aspects of special relativity and quantum mechanics.
Santilli identified since his graduate studies that, when the external terms are added, the time evolution of a quantity Q(r, p) is given by
(1.3) dQ/dt = (∂Q/∂r)(dr/dt) + (∂Q/∂p)(dp/dt) = [Q, H] + (∂Q/∂p) F = (Q, H),
where [Q, H] are the Poisson-Lie brackets. The huge technical difficulties are then set by the fact that, when the brackets [Q, H] of the truncated equations are extended to the brackets (Q, H) of the true analytic equations, there is the loss of any possible algebra, let alone all Lie algebras, in the brackets of the time evolution because the new brackets (Q, H) violate the conditions for the characterization of an algebra (the (distributive and scalar laws).
The loss of all algebras in the time evolution then causes the irreconcilable inapplicability of all Hamiltonian methods and theories developed in the 20-th century, including special relativity and quantum mechanics.
Rather than being discouraged by this occurrence, in the 1960s Santilli set as his main research goal the developement covering mathematical and physical theories suitable for the implementation of Lagrange and Hamilton analytic conception of nature while restoring an algebnra in the b rackets of the time evolution.
This presentation is essentially a review of Santilli's studies conducted since that time. As he puts it in his works: Quantitative sciences will never admit final theories. No matter how beautiful any given theory may appear, its structural generalization is only a question of time.
1.2. INSUFFICIENCIES OF SPECIAL RELATIVITY
Santilli has repeatedly stated in his writings that special relativity has a majectic axiomatic structure, for which reason he assumed said axioms for his covering relativities.
However, a widespread belief in the physics of the 20-th century has been that special relativity is valid under whatever conditions exist in the universe, to such an extent that the universe has been often adapted to verify special relativity, rather than adapting the theory to physical reality, with consequences that can only be qualified as characterizing a serious scientific obscurantism.
An important contributions made by Santilli in physics has been the identification of:
1) The conditions of clear validity of special relativity, given by the conditions originally conceived by the founding fathers, namely, for point-particles and electromagnetic waves propagating in vaccuum (empty space) or, equivalently, by all conditions in which particles can be well abstracted as being point-like, such as the electron in the hydrogen structure, particles in accelerators, and many other systems;
2) The condition of mere approximate character of special relativity, given by all conditions of particles at mutual distances equal or smaller than their wavepacket or charge distributions or, equivalently, for the motion of particles and electromagnetic waves within physical media, such as liquids, atmospoheres, chromospheres or the hyperdense media inside hadrons, nuclei and stars. These conditions cause mutual penetrations of wavepackets and charge distributions under which particles cannot be effectively approximated as being dimensionless points due to contact, nonlinear, nonlocal and non-Hamiltonian effects expected from Theorem 1.1 and other reasons reviewed in Section 3. In particular, special relativity can only be approximately valid for the structure of hadrons, nuclei and stars;
3) The conditions of inapplicability of special relativity (and not violation because the theory was not conbceived for that), such as the classical representation of antimatter (see Section 1.4), irreversible systems such as energy releasing processes, due to the strictly reversible character of special relativity compared to the strict irreversibility over time of the processes considered, and other conditions recalled in Section 3.
It shoudl be indicated that Albert Einstein identified quite clearluy in his writings the above indicated Conditions 1) for the applicability of his studies. The extension of special relativity to conditions dramatically beyond those identified by Einstein without a serious scrutiny has been perpetrated by Einstein's followewrs, who are indeed responsible for the scientific obscurantism indicated earlier and documented in more details in the rest of this presentation.
1.3. INSUFFICIENCIES OF GENERAL RELATIVITY
Unlike his view on special relativity, Santilli believes that Einstein's conception of gravitation via a curved space, despite its unquestionable mathematical beautiy, is one of the most controversial theories in history, with fundamental, yet unrestlved physical inconsistencies.
This severe view is motivated by various quantitative studies indicated in more details in Section 3. At this introductory stage, we recall Santilli's confirmation that the Riemannian geometry provides a good mathematical description of gravitys, but Santilli is unable to accept space as being truly curved by gravitation in the actual physical sense because of:
1) The impossibility of representing with curvature the weight of bodies when in stationary conditipons;
2) The impossibility of representing with curvature the free fall of bodies along a straight radial line;
3) The absence of curvature in the bending of light when passing near a celestial body, since that curvature is due to Newtonian attraction, rather than curvature of space as we shall see in Section 3, and other reasons.
At a deeper level, it should be recalled that special relativity is physically consistent because it verify the crucial condition of invariance over time, namely, the prediction of the same numerical values under the same conditoions but at different times, which invariance is ultimately due to the canonical-Hamiltonian structure of the theory and to its invariance under the Poincare' symmetry.
By contrast, Santilli has proved that the Riemannian geometry does not yield numerical values invariant over time because of the well known fact that the conception of gravitation on a curved space requires a "covariance", rather than a strict invariance, with consequential alteration of numerical values under the same conditions at different times.
Additionally, the predictions of special relativity under given conditions are unique. By contrast, Santilli has shown that the numerical prediction of general relativity for given conditions are not unique in view of the well known fact that general relativity is a nonlinear theory whose solution requires one or another approximation. It then follws that the numerical predictions depend on the selected expansion as well as the selected parameter for a given expansion.
Santilli has also shown that: general relativity violates the fifth identity of the Riemannian geometry, the Freud identity, for the case of neutral bodies (due to the lack of a source tensor in the exterior problem in vacuum); general relativity is incompatible with quantum electrodynamics (also because of the lack of a source tensor in vacuum); general relativity verifies the Theorems of Catastrophic Mathematicxal and Physical Inconsistencies for Noncanonical or Nonunitary Theories (Section 3.9); and the theory has other basic unrestolved problems generally ignored by researchers in the field, thus fueling the indicated scientific obscurantism.
1.4. INSUFFICIENCIES OF EINSTEIN'S THEORIES FOR ANTIMATTER
Another reason for the scientific obscurantism of the 20-th century is that special and general relativities were widely believed to apply for all possible conditions existing in the universe, while in reality they are unable to provide a valid classical representation of antimatter,
In fact, said theories can solely represent antimatter via the change of the sign of the charge. Consequently, said theories provide no distinction whatsoever between neutral bodies made up of matter and antimatter. Even when considering charged particles, quantization leads to inconsistencies, due to a resulting "particle" with the wrong sign of the charge, rather than the charge conjugated antiparticle.
In Santilli's words: One of the biggest scientific imbalances of the 20-th century has been the treatment of matter at all possible levels of study, from Newton to second quantization, while antimatter was solely treated at the level of second quantization. Hence, he decided to resolve this historical imbalance by discovering a new theory of antimatter that, as it is the case for matter, is applicable at all levels of study from Newtonian mechanics to second quantization, and he did indeed achieve such a goal, as we shall see in Section 3.7.
1.5. INSUFFICIENCIES OF QUANTUM MECHANICS
Santilli has repeatedly stated that quantum mechanics has made historical contributions to manking, by possessing a majectic axiomatic structure he assumed for the construction of hadronic mechanics, besides having an impressive body of expermental verifications under the conditions of its original conception and construction.
Despite these achievements, physics is a discipline that will never admit a final theory valid to the end of time. In fact, Santilli became a physicist because of authoritative doubts on the final character of quantum mechanics expressed during his high school years even in the Italian press for the general public. In fact, with the passing of time, we had the following authoritative voices of doubt:
A) The view by Albert Einstein on the "lack of completion" of quantum mechanics (in fact, Santilli constructed hadronic mechanics precisely as a "completion" of quantum mechanics in honor of Albert Einstein);
B) The doubts expressed by Enrico Fermi as to whether quantum mechanics holds in the interior of mesons (Santilli quoted repeatedly Fermi's doubt as being at the foundation for his studies on the structure of hadrons);
C) The limitations of quantum mechanics voiced by Werner Heisenberg, one of the very founders of the mechanics, from the linear character of the theory compared to the evident nonlinearity of the physical world (Santilli corresponded with Heisenberg on this topic prior to heisenberg's death in 1976);
D) The authoritative doubt voiced by Paul M. Dirac, another major founder of quantum mechanics, on the need for a revision of the theory permitting convergent perturbative expansions (Santilli met Dirac in Florida in 1982 to discuss the capability of hadronic mechanics to turn divergent quantum series into convergent forms, as reported by Santilli in his books);
E) The arguments by various philosophers of science on the need to surpass quantum mechanics with broader theories, such as Karl Popper, who was a strong supporter of Santilli's proposal to build the hjadronic covering of quantum mechanics, as stated in the Preface of his last book of 1978; and other doubts.
With the passing of time, these authoritative doubts were first ignored; then the authors were discredited via the abuse of academic authority, including the discreditation of Heisenberg, Dirac, Popper and other famous scientists for the lack of aliognment of their research with the predominant politicxal lines of the academic time; and any additional qualified doubt was prohibited to appear in print in the journals of leading physical societies, while its appearance in the press was opposed or discredited.
This evident organized manipulation of scientific knowledge and suppression of scientific democracy of qualified inquiries for personal interests lead to the widespread assumption in the last part of the 20-th century that quantum mechanics (and its Galilean and special relativity backgrounds) are the final theories for all possible conditions existing in the universe to the end of time, resulting in a manifest scientific obscurantism of historical proportions.
It is a duty duty of future historians to identify the reasons for the suppression of these authoritative doubts, as well as the responsibilities by leading academic institutions and governmental agencies funding the research, by identifying the origination of the rather universal trend of adapting all possible conditions in the universe to verify quantum mechanics and its underlying relativities.
A notorious exception is that by Santilli who honored the indicated authoritative doubts, conducted comprehensive mathematical, theoretical and experimental research on the limitations as well as the surpassing of quantum mechanics in a way completely oblivious to organized ascientific interests, and did indeed change the history of physics, as we shall see.
To begin our review in the field, another major scientific contribution by Santilli has been the restoration of a serious scientific process on quantum mechanics and its underlying relativities as follows:
1) A theory is said to be exactly valid for given conditions when it represents the totality of the physical data from primitive axioms without adulterations (such as throwing into the equations unknown parameters, arbitrary functions, and the like). This is the case for the structure of the hydrogen atoms, particles in accelerators, crystals, and numerous other systems. By analyzing the local-differential topology and mathematics underlying the theory, Santilli has confirmed that the conditions for the exact validity of quantum mechanics are the same as those for special relativity (as expected from the deep synergy of these theories), namely, quantum mechanics can be safely assumed to be exactly valid for particles and electromagnetic waves propagating in empty space or, more generally, for particles at mutual distances sufficient bigger than their size and/or charge distribution to allow their effective point-like abstraction.
2) A theory is said to be approximately valid when it does not represent all experimental data (this is the case for nuclear physics indicated below), or the representation of experimental data requires parameters and/or arbitrary functions that are then fitted from the data themselves (this is the case for numerous particle events). In particular, Santilli has proved that said arbitrary parameters and/or functions are, in reality, a direct measure of the deviations of the basic axioms of the theory from the system at hand. Numerous illustrative examples in both quantum mechanics and quantum chemistry were then worked out (see the Sections 3 and 4).
3) A theory is said to be inapplicable (rather than "violated") when the parameters thrown into the equations are incompatible with the basic axioms, or the does not admit any quantitative representation at all of experimental data.
Illustrations suitable for these introductory lines are the following:
3A) The use of four parameters necessary for the representation by quantum mechanics of the experimental data via the Bose-Einstein correlation (called "chaoticity parameters") is prohibited by quantum axioms, because the two point correlation function for a two-dimensional Hermitean (thus diagonal) operator could at best admit two parameters (the additional two parameters would be off-diagonal, thus against the Hermiticity of the Hamiltonian);
3B) Quantum mechanics is inapplicable for the synthesis of the neutron from a proton and an electron as occurring in stars because, in this case kept quite secrt by academia, the Schroedinger equation becomes inconsistent, an occurrence that is the historical motivation for the very birth of the covering hadronic mechanics, as we shall see;
3C) Santilli also proved that quantum mechanics is inapplicable for all processes that are irreversible over time, such as nuclear fusions, becausequantum mechansics is reversible over time, thus admitting the time reversal event (such as the synthesized nucleus spontaneously decomposing itself into the original two nuclei) with embarrassing violations of energy conservation, causality and other basic laws.
By looking in retrospect at a lifetime of research, we can quote Santilli's statement that: The selection of the appropriate generalization of quantum mechanics for physical conditions more complex than those of its conception and experimental verification, should indeed be the subject of scientific debates, but the aprioristic assumption of quantum mechanics as being exact for all conditions existing in the universe is ascientific, amoral and asocial particularly when ventured by physicists at leading academic institutions.
1.6. INSUFFICIENCIES OF NUCLEAR PHYSICS
The contributions of quantum mechanics to nuclear physics are well known, the most notorious being the atomic bomb and nuclear power plants. Santilli points out that these events deal with fission processes whose debris admit a good approximation as being point-like, thus allowing quantum mechanics to be effective.
As a result of said historical achievements, quantum mechanics was assumed throughout the 20-th century as being exactly valid for all possible nuclear structures and processes. Yet, Santilli pointed that quantum mechanics cannot possibly be exactly valid for fusion processes, since the theory is reversible over time. Thus, jointly with the probability of nuclear syntheses of two nuclei into a third, N1 + N2 → N3 plus energy, quantum mechanics admits a finite probability for the spontaneous time reverrsal reaction
(1.4) N3 → N1 + N2
in fragrant disagreement with the conservation of energy and other laws, trivially, because the probability amptlitude does not depend explicitly on time.
With the understanding that the approximate validity of quantum mechanics in nuclear physics is out of question, Santilli believes that one of the most pernicious manifestations of the scientific obscurantism of the 20-th century existed in nuclear physics, due to the religious assumption of the exact validity of quantum mechanics in the field when quantum mechanics has failed to achieve an exact representation of all experimental data of the simplest possible nucleus, the deuterium, because:
1) Quantum mechanics has been unable to represent the spin 1 of the deuterium since quantum axioms require that the sole stable bound state of two particles with spin 1/2, the proton and the neutron, must be the singlet state with spin zero;
2) Quantum mechanics has been unable to represent the magnetic moment of the deuterium despite 100 years of research and the use of all possible relativistic corrections;
3) Quantum mechanics has been unable to explain the stability of the neutron when coupled to the proton in the deuterium, since the neutron is a naturally unstable particle (when isolated) with about 14 minutes lifetime; and other insufficiencies.
The assumption of quantum mechanics as being exactly valid in nuclear physics reaches historical proportions when proffered by experts in the field from authoritative academic institutions, or by editors of leading physics societies, when one consider that the huge deviations of quantum mechanics from the experimental data of large nuclei, such as the zirconium.
Santilli qualifies as distressing the inability by quantum mechanics to reach a serious understanding of the nuclear force, because quantum mechanics is strictly Hamiltonian, as indicated above. Hence, all research over the past century has been studiously restricted to represent the nuclear force with a potential. The impossibility of representing experimental data then forced the addition of more and more potentials to the extreme that nuclear forces have recently reached up to 35 different potentials without achieving the needed exact representation,
(1.5) H = p2/2m + V1 + V2 + V3 + V4 + V5 + V6 + V7 + V8 + V9 + V10 + + V11 + V12 + V13 + V14 + V15 + V16 + V17 + V18 + + V19 + V20 + V21 + V22 + V23 + V24 + V25 + + V26 + V27 + V28 + V29 + V30 + V31 + V32 + + V33 + V134 + V35 + ...
To express his distress, Santilli states: There is a limit in the political manipulation of scientific knowledge and its adaptation to preferred theories, rather than adapting the theories to physical reality no matter how beloved the theories are, beyond which limit all credibility is lost to such an extent of raising issues of scientific ethics and accountability, particularly when the manipulation is perpetrated under public financial support. In fact, the insufficiency of a potential to represent nuclear forces squarely brings into focus Santilli's Theorem 1.1. on the origin of nonconservative / nonpotential forces at the very structure of matter, thus including nuclear structures.
Above all, Santilli has never accepted quantum mechanics to be exactly valid for nuclear physics because its basic symmetries, the Galilei and the Poincare' symmetries, solely apply for Keplerian systems, thus requiring a nucleus, and states: Quantum mechanics cannot possibly be exactly valid for nuclear structures because nuclei do not have nuclei, as a consequence of which the basic Galilean and Poincare' symmetries must be broken, thus causing incontrovertible deviations from quantum axioms.
As we shall see in Section 3, the "completion" of quantum mechanics into a covering mechanics achieving an exact representation of nuclear data permits the prediction and quantitative treatment of new clean energies so much needed by our society. Hence, the resolution of the approximate character of quantum mechanics in nuclear physics has major societal, let alone physical relevance.
By following Santilli, we can then again state that the selection of a mechanics more adequate than quantum mechanics for nuclear structures should indeed be the subject of scientific debates, but the aprioristic assumption of quantum mechanics as being exactly valid in nuclear physics creates serious problems of scientific ethics and accountability (with inevitable legal overtones).
1.7. INSUFFICIENCIES OF PARTICLE PHYSICS
Santilli believes that the biggest scientific obscurantism exists in particle physics with particular reference to claimed "experimental results" for high and very high energy particle collisions, and/or deep inelastic scattering, that he calls experimental beliefs.
The argument is that all these data are based on the use of the conventional potential scattering theory, namely, a theory based on the religious assumption that particles remain point-like also at very high energy collisions (a condition necessary to apply quantum mechanics) and, as such, the particles solely experience action-a-a-distance interactions derivable from a potential.
However, hadrons have in reality an extended and hyperdense charge distribution and even the electron has an extended wavepacket irrespective of its point-like charge. It then follows that the conventional, potential scattering theory can only be approximately valid for high energy scattering experiments, since it is notoriously unable to incorporate nonpotential effects due to mutual wave overlappings and/or deep mutual penetrations of hyperdense charge distributions. Under these premises, the approximate character of the "experimental results" cannot be dismissed without raising serious problems of scientific ethics and accountability.
We hope the reader begins to see in this way additional historical implications of Santilli's Theorem 1.1, since it requires the emergence of nonpotential forces precisely at the level of deep inelastic scatterig or collisions, as it is the case of the spaceship during re-entry in our atmosphere. But these forces are non-Hamiltonian, thus requiring a necessary nonunitary covering of the scattering theory, which is one of the primary objective of hadronic mechanics in view of its nonunitary structure.
Whatever nonunitary scattering theory emerges to be correct for high energy particle scattering experiments, it is clear that it will mandate a re-inspection of all "experimental beliefs" in particle physics to ascertain whether the results claimed under sole potential forces are exact or merely approximate, thus in need of basic revisions of the numerical results.
1.8. INSUFFICIENCIES OF QUARKS AND NEUTRINOS CONJECTURES
Santilli has always accepted SU(3)-color theories as providing the final Mendeleev-type classification of hadrons into families; has accepted quarks as being necessary for the elaboration of said Mendeleev classification; but he has never accepted quarks as being physical particles actually existing in our spacetime for numerous reasons, such as:
a) Quark can only be technically defined as purely mathematical representations of a purely mathematical internal symmetry, defined on a purely mathematical internal, complex-valued unitary space, without any possibility of being consistently definable in our spacetime (because prohibited by the Poincare' symmetry and other reasons);
b) Quarks cannot have any gravity because, as stated by Albert Einstein, gravity can be solely defined for masses in our spacetime, while quarks cannot be seriously defined in our spacetime.
c) Nuclei, atoms and molecules have required one model for their classification into family and a different, yet compatible model for the structure of each individual element of a given family, and the same occurrence is expected for the classification and streucture of hadrons.
To illustrate the basic dichotomy classification versus structure, Santilli has stated that: If one of my graduate students would ask me to supervise a thesis whereby the Mendeleev table for atoms is also used for the structure of each individual atoms of a given family, I would immediately request his/her expulsion from the department, because classification and structure are dramatically different problems, requiring dramatically different methods and theories.
In fact, the Mendeleev table was formulated via classical chemnical and other methods, while the structure of the atoms required the advent of quantum mechanics. As we shall see, we have a very similar situation for hadrons because the linear, local and Hamiltonian character of quantum mechanics is effective for the classification of hadrons under their point-like approximation, but the use of the same mechanics for structure problems has been shown to be inadequate due to inevitable nonlinear, nonlocal and non-Hamiltonian effects occurring within hyperdense media inside hadrons.
Similarly, Santilli never believed that the neutrinos are physical particles in our spacetime for numerous reasons, the first being the fact that the neutrino is assumed to be emitted during the synthesis of neutrons from protons and electrons inside stars,
(1.6) p+ + e- → n + ν,
while a more correct assumption should have been its absorption.
This is due to the fact that the neutron is 0.782 MeV heavier than the sum of the rest energies of the proton and the electron,
(1.7) Ep = 938.272 MeV, Ee = 0.511 MeV, En = 939.565 MeV, Eν = ?.
As a result, quantum mechanics is basically inapplicable for any quantitative treatment of synthesis (1.6) for various reasons, such as:
A) All bound states characterized by quantum mechanics (such as nuclei, atoms and molecules) must have a "mass defect," namely, the rest energy of the resulting state must be smaller than the sum of the rest energies of the constituents, resulting in the familiar "negative binding energy." By contrast, reaction (1.6) requires a kind of "mass excess," thus requiring a "positive binding energy," under which the Schroedinger and other equations of quantum mechanics become inconsistent.
B) The assumption of the "missing energy" of 0.782 MeV as being provided by the relative kinetic energy of the proton and the electron is inconsistent and untenable, because at that energy the cross section of protons and electrons is virtually null., thus prohibiting any bound state;
C) The belief that the conjugate expression
(1.8) p+ + ν† + e- → n,
where ν† denotes antineutrino (duuje to the absence in htlm language of ν-bar), is political and eually inconsistent, because the antineutrino has an identically null cross section with the proton and the electron, thus being unable to provide them the missing energy. In any case, recent theories have established that antineutrino should have a negative mass referred to a negative unit, (see Sections 2,3), thus requiring, rather than providing energy for the neutron synthesis.
The advent of the standard model has caused additional, rather serious, unresolved problems because Fermi's original conception of one massless and chargeless neutrino and its antiparticle had to be first extended to three different neutrinos and their antiparticles without any serious identification of their differences; then this enlargement had to be further enlarged to admit that neutrinos have masses; then the latter enlargement had to be further broadened with the additional belief that neutrinos have different masses; then the latter assumption had to be further modified with the conjecture that neutrinos "oscillates" (that is, change from one into the other); with the expectation of additional unverifiable conjectures introduced to bypass the problems unsolved by the preceding conjectures, yet under very large public funds dispersed at major international laboratories on these pure theoretical theologies without any serious scrutiny by society, thus confirming the ongoing scientific obscurantism.
Any denials of the need for a basic re-inspection of physical laws for the most fundamental syntheses in nature, that of the neutron, can only raise serious problems of scientific ethic s and accountability (also with inevitable legal overtones).
Santilli states: Until I live, I will refuse to accept that massive particles, as neutrinos are believed nowadays to be, can traverse entire planets and stars, thus passing through an enormous number of nuclei, without any collision. Instead of accepting such a theology, I will look for alternative theories more plausible than that of the neutrinos, and so, in fact, he did, by introducing his theory of "longitudinal" impulses propagating through the ether as a univbersal substratum, thus explaining the lack of collision (see Section 3).
Unreassuringly, Santilli has also stated that: Quarks and neutrinos have been claimed to exist as physical particles in our spacetime by organized high ranking academic interests because their assumption is essential to preserve the validity of special relativity and quantum mechanics.
In any case, the various claims of leading particle laboratories to have "discovered" or "detected" this or that quark is extremely anti-scientific for me because the correct scientific statement should have been that of having detected physical particles in our spacetime "predicted" by quark conjectures, with the understanding that the same particles could be predicted by other conjectures.
In the final analysis, the conjecture that quarks are physical particles in our spacetime prohibits the study of possible new clean energies because quarks must be assumed as being permanently confined in the interior of hadrons, while all energies obtained from nuclear, atomic and molecular structures are based on the capability of extracting the constituents free.
1.9. INSUFFICIENCIES OF QUANTUM CHEMISTRY
With the acknowledgment that quantum chemistry has also made historical contributions to society, beginning with the time of his graduate studies in the 1960s, Santilli never accepted quantum chemistry as a final discipline for numerous reasons he has identified in his works. For instance, he states that:
The fundamental quantum chemical notion of valence bond, as presented in the 20-th century literature, is a pure nomenclature without quantitative content because, to be quantitative, the notion should:
1) Identify clearly the force between two identical valence electrons;
2) Prove that such a firce is attractive, as an evident necessary pre-requisite to claim the bond needed for a molecule; and
3) Prove that such a clearly identified clearly attractive force verifies indeed experimental data on molecular structures.
These conditions are impossible for quantum chemistry, because two identical electrons must "repel" each other according to quantum mechanics, and they cannot possibly "attract" each other.
Therefore, Santilli set his goal to achieve the missing quantitative notion of valence, and he did achieve it, as we shall see in Section 4, giving birth to the new discipline of hadronic chemistry
Santilli has also identified additional structural problems of quantum chemistry, among which most visible is the prediction (verified by one of his graduate students) that all substances are paramagnetic, in great disagreement with evidence establishing that only certain substances are paramagnetic.
This insufficiency can be verified with the hydrogen molecule that is indeed diamagnetic. The origin of the problem rests in the absence of a clearly identified, sufficiently "strong" valence bond among the pair of valence electrons of the H2 molecule, as a result of which the orbitals of individual hydrogen atoms remain essentially independent, thus available for a joint polarization via an external magnetic field, contrary to evidence.
Santilli had another graduate student prove that, under the current notion of valence, there is no reason to have the sole molecule H2, since it is possible to bond together three, four or more hydrogen atoms, contrary to evidence. The origin of this additional insufficiency is, again, the lack of a "strongly" attractive valence bond restricting the correlation to valence electron "pairs" only, thus allowing the bonding of additional electrons, contrary to evidence (as we shall see in Section 4, the species H3, H4 at times detected in gas chromatography have been proved by Santilli to have a bond other than that of valence).
Santilli proved additionally that quantum chemistry cannot be exactly valid for the study of chemical reactions, by showing that, jointly with the prediction of the synthesis of the water molecule H2 + O → H2O, quantum chemistry admits a finite probability for the time reversal event, the spontaneous disintegration of the water molecule into its original constituents,
(1.9) H2O → H2 + O,
in dramatic of the principle of conservation of the energy. The reason is well know, but kept a great secret in advanced chemistry departments and laboratories, namely, the fact that quantum chemistry is a theory reversible over time, while chemical reactions, such as the synthesis of the water molecule, are strictly irreversible processes.
It is then evident to all serious scholars outside academic politics that quantum chemistry cannot possibly be the final theory for chemistry, the most serious limitations occurring for chemical reactions. Of course, the applicable new chemistry is open to scientific debates, but the denial of its need can only raise issues of scientific ethics and accountability (again, with inevitable legal overtones).
1.10. INSUFFICIENCIES OF BIOLOGY
Among all sciences of the 20-th century, that considered most distressful by Santilli is biology treated via quantum mechanics. In fact, he writes: Had quantum mechanics be applicable to biological processes, my body should be perfectly rigid and perfectly eternal.
This insufficiency is due to the well known incompatibility of quantum mechanics with the deformation theory (since deformations would cause the breaking of the central pillar, the rotational symmetry), as a result of which quantum mechanics is ideally suited to represent rigid structures such as crystals. Additionally, the insufficiency poriginates from the reversibility of quantum mechanics over time, compared to the finite life of all biological processes.
Particularly distressing for Santilli is the study of the DNA structure via the elementary mathematics of the 20-th century, such as conventional numbers dating back to pre-biblical times, while the complexity of biological processes is simply beyond our imagination at this time.
1.11. INSUFFICIENCIES OF ASTROPHYSICS AND COSMOLOGY
According to Santilli, the climax of the scientific obscurantism of the 20-th century can be seen in astrophysics and cosmology, because these disciplines have seen true extremes in the adaptation of the universe to verify Einsteinian doctrines without a serious scrutiny.
To begin, the study of the antimatter component of the universe, the consequential expected existence of antigravity between matter and antimatter and related topics, have been systematically ignored because notoriously not compatible with Einsteinian doctrines (Sections 2.4 and 3.7).
Additionally, Santilli believes that the ongoing views on the expansion of the universe, the acceleration of the expansion with the distance, and the so-called "big bang" theory, are a consequence of the intent of preserving the constancy of the speed of light throughout the universe. On serious scientific grounds, we can say that the speed of light is indeed a constant, but solely under the conditions established by experiments until now, when propagating in vacuum conceived as a totally empty space.
The widespread claim of "the universal constancy of the speed of light" is a political, rather than a scientific statement when ventiured without the crucial words "in vacuum", because disproved by evidence when dealing with propagation of light within physical media. It is today well established that the speed of electromagnetic waves C = c/n has the constant value c only in vacuum, while having otherwise a locally varying character depending on the characteristics of the medium in which it propagates represented by the index of refraction n. Santilliu argues that at intergalactic distances, space cannot be considered empty, thus voiding the foundations of current cosmological theologies.
Above all, one of Santilli's major contribution in astrophysics and cosmology has been the focusing of the attention on ether as a fundamental universal medium (substratum) with very high energy density. A star at its initiation synthesizes from hydrogen a very large number of neutrons estimated to be of the order of 1050 neutrons per seconds or more. But the synthesis of a neutron requires 0.782 MeV, as noted above. According to orthodox views the missing energy is provided by the star environment. However, in this case a star could never initiate to produce light, since at its initiation the star would lose (rather than produce) energy at the rate of 1050 MeV per seconds or more.
The sole possibility for a scientific solution of this fundamental problem is the ether, whose study is seen by Santilli as the ultimate frontier of knowledge, with possible advances simply beyond our most vivid imagination at this time, such as possible longitudinal communications through space at speeds millions of times bigger than that of the transversal electromagnetic waves, or travel to the stars at unrestricted speeds without fuel tanks because the needed propulsion and energy may be available everywhere in the ether, provided, of course, we have basically new theories suitable for the study of these advances.
As we shall see, one of the ultimate motivations for the construction of hadronic mechanics has been to provide means for quantitative studies of possible interchanges between the ether as a universal substratum and the visible universe, a study definitely not possible with quantum mechanics.
1.12. INTRODUCTORY READINGS
Scholars with a serious interest in acquiring an in depth knowledge of Santilli's discoveries, are suggested to initiate their study with introductory readings, rather than with technical treatments, since the latter may appear to be disconnected from the larger scientific edifice.
A first recommended reading is that on the insufficiencies of the 20-th century theories available in the
Forum on Old Theories
A comprehensive technical presentation of said insufficiencies can be found in the monograph available for free download in pdf format
Hadronic Mathematics, Mechanics and Chemistry, Volume I: Limitations of Einstein's Special and General Relativities,
Quantum Mechanics and Quantum Chemistry
R. M. Santilli, International Academic Press (2008)
Santilli has been one of the firsts to present in 1981 various arguments according to which quarks cannot be physical particles in our spacetime. See the paper
An intriguing legacy of Einstein, Fermi, Jordan and others:
The possible invalidation of quark conjectures
R. M. Santilli,
Found. Phys. Vol. 11, 384-472 (1981).Br>
A detailed technical treatment of the insufficiencies of 20-th century theories and a denunciation of their lack of addressing dated 1984 was presented by Santilli in the book also available in free pdf download
Ethical Probe of Einstein's Followers in the USA: An Insider's View
R. M. Santilli, Alpha Publishing (1984)
The related 1,315 pages long documentation dated 1985 is also available in free pdf download from
Documentation of the Ethical Probe R. M. Santilli, Alpha Publishing (1985)
The Foundation is attempting to secure copies of Santilli's personal documentation following 1985 that has been donated to a European Institution.
2. SANTILLI'S DISCOVERIES IN MATHEMATICS
2.1. FOREWORD
Santilli has repeatedly stated that: The origin of protracted controversies or unsolved problems in physics, chemistry and biology, is generally due to the use of mathematics basically insufficient for the quantitative treatment of the problem at hand, with consequential need to develop new appropriate mnathematics.
Most of the insufficiencies of the 20-th century theories identified in the preceding section see their origin precisely in the lack of adequate mathematics, such as: the reconstruction of an algebra in the brackets of the time evolution with external terms, Eq. (1.3), clearly requires the development of a suitable new algebra other than Lie algebra; the classical and operator treatment of nonlinear, nonlocal and non-Hamiltonian interactions for extended particles at short mutual distances clearly requires a mathematics broader than that effective for conventional Hamiltonian and quantum theories; the insufficiencies of curvature to represent gravitation, combined with the inabilities by general relativity to reach a grand unification and a quantum version of gravity dating back to Einstein's times without solution, are a clear manifestation of the need for a more appropriate geometry for gravitational events; and the same occurs for other problems whose solution is impossible with the mathematics of the 20-th century.
Santilli has also states repeatedly in his writings that: There cannot be a really new theory without a really new mathematics, and there cannot be a really new mathematics without new numbers.
Hence, as a theoretical physicist, he devoted the majority of his time to the search of new numbers, and then to the construction of new mathematics based on them. Discoveries in physics, chemistry, biology, astrophysics and engineering required the minority of his time.
To understand the mathematical discoveries outlined below, one should keep in mind the main problem investigated by Santilli. Recall from Section 1.1 the legacy of Lagrange and Hamilton according to which the representation of nature requites the knowledge of two quantities, a Lagrangian or a Hamiltonian and the external force F(t, r, p, ...). Recall also from Eq. (1.3) that the presence of the external forces causes the loss of all algebras in the brackets of the time evolution of physical quantities, thus preventing the construction of physically meaningful covering theories.
Hence, Santilli set his research goal to identify an identical reformulation of Hamilton's equation (1.2) depending on a second quantity, besides the Hamiltonian, capable of restoring an algebra in the brackets of the time evolution and that algebra is a covering of the Lie algebra.
After extensive research and the systematic investigations of all possible alternatives, Santilli finally assumed the representation of Lagrange's and Hamilton's external forces via a generalization of the basic unit E*(t, r, p, ...). All other alternatives failed because of their lack of invariance over time, that is, the inability to predict the same numerical values under the same conditions at different times, thus being physically inconsistent.
By comparison, the unit is the most fundamental invariant of all theories, thus being the best solution for the preservation of the same time invariance as that of the truncated analytic equations. However, the generalization of the basic unit requires a corresponding, progressive, and systematic generalization of the totality of the mathematics of the 20-th century, and this explains the dimension as well as novelty of Santilli's mathematical discoveries.
In this section we recall what is today known as Santilli mathematics (at times also called hadronic mathematics to indicate the mathematics underlying hadronic mechanics), namely, numerical fields, vector and metric spaces,geometries, algebras and groups, etc., characterized by a basic unit E*(t, r, p, ...) that, besides being nowhere singular, has otherwise an unrestricted functional dependence on all needed local variables. The application of Santilli mathematics for the resolution of Lagrange's and Hamilton';s legacy is outlined in Section 3.
Mathematicians should be aware that all mathematical discoveries outlined in this section originated from specific physical needs following clear insufficiencies of the pre-existing mathematical and physical methods. Mathematicians should also keep in mind that Santilli has been a member of the Department of Mathematics of Harvard University from 1978 to 1983 under DOE financial support, thus having all qualifications for mathematical discoveries even while being a theoretical physicist. Nevertheless, mathematicians should keep in mind that, except a number of papers written in pure mathematics language for mathematicians, numerous mathematical discoveries were presented by Santilli in papers intended for physicists and published in physics journals, the understanding being that their re-elaboration in the language of pure mathematics is elementary.
In this mathematical section, the conventional associative multiplication "ab" of two numbers, matrices, operators, etc. will be denoted with the sumbol "a x b" in order to differentiate it from various new multiplications discovered by Santilli that are still associative, yet more general than the trivial multiplications ab.
2.2. DISCOVERY OF NEW NUMBERS
2.2A. Discovery of isonumbers (1983)
Numbers are at the foundation of all quantitative sciences, since, by definition, the latter require mathematical elaborations predicting numbers that can be verified with experiments. For various topological and other technical reasons, experimental measurements requires the adopted "ordinary numbers" (hereon referred to those with characteristic zero and denoted with the letter n) to verify the axioms of a numerical field F(n, x, E) with associative multiplication n x m, (left and right) multiplicative unit E, E x n = n x E = n for all elements n of the set F, addition n + m = p ε F and additive unit 0, 0+n = n+0 = n.
The achievement of the modern number theory requires contributions from the best scientific minds in history, including Gauss, Legendre. Jacobi, Cauchy, Lebesque, Diriclet, Hamilton, Cayley, and many others.
A major historical effort was dedicated to the classification of all possible numbers, that is, all possible sets verifying the axioms of a numerical field. By the middle of the 20-th century, it was universally believed in mathematics that the classification of all ordinary numbers (again, those with characteristic zero) had been achieved with the results that all possible ordinary numbers are given by the real numbers, complex numbers and quaternionic numbers. Octonions do not qualify as numbers because they violate the associativity of the multiplication (m x n ) x p = m x ( n x p).
As part of his Ph. D. in theoretical physics in the late 1960s at the University of Torino, Italy, Santilli set up his research goal of achieving a generalization-covering of quantum mechanics for which, to avoid the illusion of a real generalization, he needed numbers more general than those used in quantum mechanics, such as the real and complex numbers.
The difficulty of Santilli's task was that, on one side, very authoritative mathematicians claimed emphatically that all ordinary numbers verifying the axioms of a numerical field had been classified while, on the other side, Santilli needed new numbers verifying indeed said axioms to avoid physical inconsistencies identified later on.
With great scientific audacity, and based on the conviction that mathematics will never admit final formulations, Santilli ignored all authoritative claims and set himself up to review the foundations of number theory. His position at the Department of Mathematics of Harvard University proved to be instrumental, not because of any help by departmental colleagues, but because their skepticisms that reinforced his determination.
In this way, Santilli first discovered that the axioms of a numerical field do not require that the multiplicative unit be necessarily the number E = +1 dating back to pre-biblical times but used in pure mathematics up to the 20-th century, since the left and right multiplicative unit can be an arbitrary positive-definite quantity E* = 1/T > 0 generally outside the original set F(n, x, E), provided that the multiplication is suitably re-defined in the form n x* m = n x T x m, under which E* remains indeed the correct left and right unit, E* x* n = n x* E* = n for all elements of the set.
Santilli then proved that, under the above assumptions for the multiplication and its unit while keeping the conventional addition and its unit, all axioms of a field were verified even when ethe new unit E* is not an element of the original field F, in which case the new numbers are written n* = n x E*. We reach in this way new numbers and fields for which Santilli suggested the name of isonumbers and isofields. from the Greek meaning of preserving the original axioms. They are known today as Santilli¹s isoreal, isocomplex and isoquaternionic numbers, or generically isonumbers, the new unit E* = 1/T > 0 is called Santilli isounit, its inverse T is called the isotopic element, and the new multiplication a x* b between two generic quantities a, b is called isomultiplication. The new sets F* are called Santilli isofields and are generally written in the form
(2.1) F*(n*,x*, E*): E* = 1 / T ≠ 1, n* = n x E*, n* x* m* = (n x E*) x T x (m x E*) = (n x m) x E* .
(2.2) F*(n*,x*, E*) ≈ F(n, x, E),
In short, Santilli discovered a new realization of the conventional axioms of a field permitting new physical, chemical and other applications identified in subsequent sections. When the new unit E* is outside the original set F, F*(n*,x*, E*) is valled an isofield of the first kind, and the numbers n* are called isonunmbers of the first kind. When E* is an element of the original field F, that is, an ordinary number, F*(n*,x*, E*) is called an isofield of the second kind, in which case the isonumbers of the second kind are often assumd to be the original numbers n without the multiplication by E*.
Even though isofields are isomorphic to conventional fields, as indicated by their very name and Eq. (2.2), their differences are by far nontrivial, and their scientific implications beyond our imagination at this time. For instance, when E* is an element of the original field F, we have expressions of the type
(2.3) E* = 1/3: 2 x* 3 = 18, 4 = prime number.
These results signaled one of the biggest mathematical discoveries of the 20-th century because it gave rise to momentous advances in physics, chemistry, biology and other quantitative sciences reviewed ssectsions 3, 4.
Quite symptomatically, Santilli published for the first time his isonumbers in his two historical papers of 1985 on the isotopies of Lie's theory, particularly for the structural lifting of the fundamental symmetry of physics, the rotational symmetry that, in turn, is the basis for his lifting of Galilei's and Einstein's relativities (see paper I, Eq. (30), page 30).
Lie-isotopic liftings of Lie symmetries, I: General considerations
R. M. Santilli,
Hadronic J. Vol. 8, 25-35 (1985)
Lie-isotopic liftings of Lie symmetries, II: Lifting of rotations
R. M. santilli,
Hadronic J. Vol. 8, 36-51 (1985)
A mathematically rigorous presentation of isonumbers and isofields isonumbers was then given in the 1993 paper
Isonumbers and genonumbers of dimension 1, 2, 4, 8, their isoduals
and "hidden numbers" of dimension 3, 5, 6, 7.
R. M. Santilli, Algebras, Groups and Geometries Vol. 10, 273-322 (1993).
Numerous independent papers and books have been written on Santilli¹s isonumbers and isofields (see the General Bibliography). We here merely quote the monograph written in 2001 by the Chinese mathematician Chun-Xuan Jiang that remains a significant general study in the field to this day
"Foundations of Santilli Isonumber Theory"Lie-isotopic liftings of Lie symmetries, II: Lifting of rotations
Chun-Xuan Jiang, International Academic Press (2001).
A readable presentation of Santilli¹s isonumbers in Italian is given by the paper
I nuovi numeri santilliani,
Parte I: I nuovi numeri isotopici e loro applicazioni
Michele Sacerdoti
2.2B. Discovery of genonumbers (1993)
Despite the dimension and implications of the preceding discovery, Santilli remained dissatisfied because his main objective was to reach a structural generalization of quantum mechanics suitable for the representation of energy reelasing processes such as nuclear fusions that are irreversible (that is, the time reversal images violate causality laws). Isonumbers could not allow such a generalization because they have no "
time arrow."
Hence, Santilli went back o work and re-examined the foundations of his own isotopic number theory. He discovered in this way that, in addition not to require the value +1 for the multiplicative unit, the axioms of a field do not require that the unit for the multiplication to the right be equal to the unit for then multiplication to the left, provided that all multiplications are correospondently ordered to the right and to the left, respectively.
This discovery gave rise to a broader class of new numbers (again with characteristic zero, the sole known to have physical applications at this writing), also verifying the axioms of a field, called by Santilli genonumbers in the Greek meaning that they induce a new structure. The new numbers are known today as Santilli¹s genoreal, genocomplex and genoquaternionic numbers to the right and to the left or, generically, as genonumbers..
By using the symbols Er and n xr m for the genounit and genomultiplication to the right and the symbols lE and n lx m for the genounit and genomultiplication to the left, we can write the genofields in the form
(2.4) Fr(nr, xr, Er): Er = 1 / S, nr = n x Er, nr xr mr = nl x S x mr = ( n x m) x Er,
(2.5) lF(ln, lx, lE): lE = 1 / R, ln = lE x n, ln lx lm = ln x R x lm = lE x (n x m),
(2.6) Er = (lE)c
where c is a conjugation depending on the desired application (such as Hermitean conjugation. complex conjugation, inverse, transpose, etc.) for the interconnection between the right and left settings.
Again, genofields are isomorphic to conventional fields by conception and construction. Nevertheless, the implications are by far nontrivial. For instance, by assuming that the genounits are elements of the original field F (Santilli¹s genonumbers of the second kind, otherwise they are called of the first kind), and by using the inverse for the conjugation c, a realizations Fl(n, xl, El) and lF(l, ln, lEis given by
(2.7) Er = 1 / 3, lE = 3, , 2 xr 3 = 18, 2 lx 3 = 2,
namely, not only the product of 2 time 3 does not yield the usual number 6, but the product to the right is different than the product ot the left, all in a way fully compatible with the axioms of a numerical field.
This discovery caries scientific implications greater than those for isonumbers, because genonumbers have permitted the construction of mathematically rigorous methods for the invariant treatment of irreversibility, including the study of new energies, that are not treatable with the mathematics of the 20-th century, because the latter has no "time arrow". In fact,Santilli¹s genotheories represent irreversibility via the most basic mathematical quantity, the unit, with the physical interpretation that genounits and genomultiplication to the right represent motion forward in time while genounits and genomultiplications to the left represent motions backward in time.
Santilli presented his discovery of genonumbers in his historical mathematical paper of 1993
Isonumbers and genonumbers of dimension 1, 2, 4, 8, their isoduals
and "hidden numbers" of dimension 3, 5, 6, 7.
R. M. Santilli, Algebras, Groups and Geometries Vol. 10, 273-322 (1993).
and immediately applied the new numbners in his monographs
"Elements of Hadronic Mechanics", Vol. I: "Mathematical Foundations"
R. M. Santilli, Ukraine Academy of Sciences (1993).
"Elements of Hadronic Mechanics"
Vol. II: "Theoretical Foundations"
R. M. Santilli, Ukraine Academy of Sciences (1994).
A readable presentation of Santilli's genonumbers in Italian is given by the paper
I nuovi numeri santilliani,
Parte II: I nuovi numeri genotopici ed iperstrutturali\\ e loro applicazioni
Michele Sacerdoti
2.2C. Discovery of hypernumbers (1994)
Despite the above momentous discoveries, Santilli continued to remain dissatisfied because, as he stated several times in his works and correspondence, I cannot accept the idea that the DNA code can be understood with genonumbers because, even though they do represent the irreversibility of biological processes, they cannot possibly represent how two atoms of a DNA can produce an entire organ with a very large number of constituents.
In this way the genonumbers were extended to yet new numbers today known as Santilli¹s hyperreal, hypercomplex and hyperquaternionic numbers to the right and to the left that are multivalued, namely, not only the units and products to the right and to the left are different, but the hyperunit has an ordered set of value and, consequently, the multiplication yields an ordered set of values. For instance, the hyper-lifting of example (2.7) would yield expressions of the type
(2.8) Er = {1 / 3, 4, 2, ...} = (lE)-1 , 2 xr 3 = {18, 3/2, 3, ...}, 2 lx 3 = {2, 24, 12, ...}.
It should be indicated that Santilli's hypernumbers are different than those belonging to hyperstructures because the former uses conventional operations while the latter use abstract operations. Also, Santilli's hypernumbers verify all axioms of a field, while conventional hyperstructures do not generally admit any unit at all, thus not being generally formulated over a field, with consequential severe restrictions in apphycations.
Santilli published his hypernumbers for the first time in the following also historical memoir
Nonlocal-integral isotopies of differential calculus,
mechanics and geometries
R. M. Santilli, Rendiconti Circolo Matematico Palermo, Suppl. Vol. 42, 7-82 (1996).
and then applied them to biology in the subsequent monograph
"Isotopic, Genotopic and Hyperstructural Methods in Theoretical Biology"
R. M. Santilli, Ukraine Academuy of Sciences (1997).
2.2D. Discovery of isodual numbers (1993)
Despite all the above discoveries, each of which being quite significant, Santilli remained dissatisfied because, as he put it in his works and correspondence: When I look at the stars, I feel very frustrated as a physicists for my complete inability to study whether a far away star or quasar is made up of matter or of of antimatter.
As indicated in Section 1.4, mathematical and physical methods of the 20-th century were insufficient to allow any consistent classical description of antimatter.The new iso-, geno- and hyper-numbers were insufficient to allow Santilli to reach the needed classical description of antimatter precisely because of their isomorphic to conventional numbers. In fact, charge conjugation is an anti-automorphism. Hence, a classical representation of antimatter admitting an operator image compatible with charge conjugation needs a mathematics that is anti-homomorphic or, better, anti-isomorphic to the the convenbtional mathematics of the 20-th century, including its iso-, geno-, and hyper-liftings.
When at the Department of Mathematics of Harvard University in the early, u conducted a comprehensive search in the Cantabridgean mathematics libraries and concluded that the mathematics needed for a classical representation of antimatter did not exist in the form needed by physicists, such as to yield under quantization an image equivalent to charge conjugation.
A day in February 1982 Santilli invited one of his mathematics colleagues to go with him to the mathematics library (located in the ground floor of Harvard's Science Center) and suggested him to select any desired volume by opening it at any desired page. He would prove that the mathematics of that arbitrary page of an arbitrary volume of that large mathematics library would not allow a physically consistent classical representation of antimatter. He was indeed right.
As a physicist, Santilli was forced, again, to study yet new mathematics and he was forced, again, to study yet new numbers. In this way, Satilli discovered that the axioms of a numerical field admit negative units and the resulting fields are anti-isomorphic to the conventional ones as desired. More generally he introduced a new map he called isoduality (denoted with an upper index d) consisting of an anti-Hermitean operation, e.g. for an arbitrary quantity Q(n, ...) we have
(2.9) Qd(nd, ...) = - Q†(-n†, ...),
provided that the above conjugation is applied to the totality of the elements of a given theory and all their operations. This gave rise to Santilli¹s isodual conventional, iso-, geno- and hyper-numbers, negative definite units are called isodual iso-, geno-, and hyper-units, and the corresponding multiplications are called isodual iso-, geno-, and hyper-multiplications
.
As the simplest possible illustration, consider conventional field F(n, x, 1). Then, Santilli¹s isodual field is given by
(2.10) Fd(nd, xd, 1d): 1d = -1, nd = - n†, (n x m)† = - (m† x n†).
The isoduals of iso-, geno- and hyper-numbers can be similarly constructed via isoduality (2.9).
Even though seemingly trivial, isodual numbers have their own rather deep implications requiring attention to prevent inconsistencies. For instance, the statement of having +1,000 dollars in the bank, in reality means for isodual numbers that the account is 1,000 dollars short because the number +1,000 is now referred to the basic unit -1. the isodual norm of -1,000 is negative, etc.
To illustrate the mathematical novelty here, we can report the following episode quoted by Santilli in footnotes of some of his books. in June 1996, Santilli and his wife Carla went to Palermo, Sicily, to pay their tribute to the Circolo Matematico Palermo for the publication of a special issue of their famous mathematical journal entirely dedicated to Santilli's isotopies. During that occasion, as a gesture of appreciation, the Editor in Chief of the journal, Prof. P. Vetro, located a 20 minutes opening at a mathematical conference going on in Palermo at that time and suggested Santilli to present there his new mathematics just appeared in the Rendiconti.
Santilli accepted the offer and elected to present his recently discovered isodual number theory and related mathematics by initiated his lecture with the projection in the big screen of a transparency with only the number "-1" in it and the indication that he assumed that quantity as the basic unit of his mathematics. At that view and statement, the audience went into great agitation with numerous questions from all sides, often repeated various times, to such a disarray that 20 minutes passed without Santilli being able to present any additional transparency.
Mathematicians are accustomed to write structures in an abstract, realization-free form. For this purpose Santilli suggest the use of conventional symbols F(n, x, E) for the abstract unification of all his new numbers, provided one has a knowledge of all possible realizations not only of the unit, but also for the related multiplications.
The above abstract unification would casue serious problems if use in physics,m e.g., because of mixing inadcertrently particles and antiparticles. This is the reason that in physical application it is much better to have different specific formulations for fields, isofields, genofields, hyuperfields and their isoduals since the identification of the asusmed numbers and their unit identifies the level ofd treatment and relkated applications.
We cannot close this section without an indication of yet another mathematical discovery by Santilli givenm by iso-, genop-, hyper-fields and their isoduals when the related generalized unit are admitted to have a functional. dependence with null (or infinite) value, an occurrenc of impossible conception in the 20-th century mathematics since fields are assumed to have the trivial unit + 1. Asd swe shall see in Section 3.10, this case is of particular physical relevance since Lim E* → 0 represents gravitational singularities.
To the writer best knowledge, Santilli published for the first time his isodual numbers in the historical mathematical paper of 1993
,p>
Isonumbers and genonumbers of dimension 1, 2, 4, 8, their isoduals
and "hidden numbers" of dimension 3, 5, 6, 7.
R. M. Santilli, Algebras, Groups and Geometries Vol. 10, 273-322 (1993).
"Isodual Theory of Antimatter, with Application to Antigravity, Grand Unification and Cosmology",
R. M. Santilli,Springer (2006).
A readable presentation of Santilli's isodual numbers in Italian is given by the article
I nuovi numeri santilliani,
Parte III: I nuovi numeri isoduali e loro applicazioni
Michele Sacerdoti
2.3. ISO-, DISCOVERY OF GENO-, HYPER-DIFFERENTIAL CALCULI AND THEIR ISODUALS (1996)
Santilli's main scientific objective has been the study of Lagrange's and Hamilton's legacy (Section 1.1), namely, the study of contact non-Hamiltonian interactions at all levels, from Newtonian mechanics to second quantization. besides the need for new numbers, Santilli faced another major technical obstacle, that of achieving the representation of all possible non-Hamiltonian forces via an action principle, because suich a principle is necessary for quantization. As a matetr of fact, the lack of achievement of any quantum formulation of non-Hamiltonian interactions during the 20-th century was precisely due to the lack of any consistent method for their quantization.
Again, as a theoretical physicist, Santilli was forced to study pure mathematics as a condition to formulate consistent physical theories. After decades of trials and failures, Santilli recalled in late 1995 that, Newton had to invent (with Leibnitz) the differential calculus before he was in a position to write his celebrated equations.
In this way, Santilli inspected the differential calculus and discovered that, contrary to a deeply rooted belief in pure mathematics for over four centuries, the differential calculus is indeed dependent on the assumed basic unit. Let r be the coordinate of a Newtonian particle and dr its differential. Assume the isotopic lifting of r into an isocoordinate r* = r x E*, with isounit E* = 1 / T > 0. In this case, Santilli proved that the isodifferential is given by
(2.11) d* r* = T x *d (r x I*).
If the isounit is independent from the local variable of the calculus, the differential is indeed independent from the local valuable because
(2.12) E* = 1 / T = const., d* r* = T x E* x dr = dr,
thus recovering the indicated belief in pure mathematics. However, when the isounit depends on local variable, E* = E*(r, ...), the above simplification is no longer possible because
(2.13) d* r* = T x d [r x E*(r, ...)] = dr + T x r x dE*(r, ...).
This marked the discovery of a structural generalization of the differential calculus that, as illustrated by the momentous implications outlined in this presentation, is indeed yet another mathematical discovery of clear historical proportions, today known as Santilli's iso-, geno-, hyper-differential calculi for matter and their isoduals for antimatter,
The geno-, and hyper-differential calculi for matter and their isoduals for antimatter are quite intriguing, particularly for the correct treatment of irreversible processes.
These various new calculi were first published in the historical memoir of 1996 and in all subsequent works
Nonlocal-integral isotopies of differential calculus,
mechanics and geometries
R. M. Santilli, Rendiconti Circolo Matematico Palermo, Suppl. Vol. 42, 7-82 (1996).
2.4. DISCOVERY OF ISO-, GENO-, HYPER-, SPACES AND THEIR ISODUALS (1983).
As it is well known, all quantitative theories must be defined on a representation space, such as the Euclidean or Minkowski or Riemannian space that, in turn, is defined over a field of numbers. It is evident that the generalization of ordinary numbers generated a corresponding liftings of conventional spaces, today's known as Santilli's iso-, geno, and hyper-spaces for matter and their isoduals for antimatter.
The implications of these broader spaces are far reaching, as we shall see. Consider the conventional, (3+1)-dimensional Minkowski space M(r, m, E) with spacetime coordinates r, metric m = Diag. (1, 1, 1, - c2) and invariant (ri x mij ri) x E where E is unit of the Lorentz symmetry, E = Diag. (1, 1, 1, 1). Then, the isounit, isometric, and isoline element on Minkowski-Santilli isospace are given by
(2.14) M*(r*, m*, E*): E* = 1 / T = Diag. ( T12, T22. T33, T44) =
= Diag. ( n12, n22, n32, n42) > 0,
(2.15) m* = T x m = (Tij x mjk) = Diag. (1/ T12, 1/T22, 1/T33, - c2 /T44) =
= Diag. (1/ n12, 1/n22, 1/ n32, - c2/n42),
(2.16) r*2* = ( r*i x* m*ik x* r*k) x E* = (r12/ T12 + r22/T22 + r32/T33 - t2 x c2/T44) x E* =
= ( r12/n12 + r22/n22 + r32/n32 - t2 x c2/n42) x E* ε F*(n*, x*, E*),
where: we have shown the most general possible, diagonal realization of Santilli's isounit and its realization in physics via the so-called characteristic quantities nk, k = 1, 2, 3, 4; r4 = t x c; and the notation rk2, k = 1, 2, 3, 4, denotes the square of rk.
The implications can only be qualified as historical, as shown in the rest of this presentation. We only mention the representation for the first time in scientific history via a metric of the actual dimension of particles via the space-component n2k, k = 1, 2, 3 (normalized to the value 1 for the perfect sphere), the representation of its density characterized by n42 (normalized to the value 1 for the vacuum), and the representation of arbitrary speed of light C = c /n4, where n4 is the familiar index of refraction.
A fundamental property of Santilli isospaces is that, by conception and construction, they are isomorphic to the original spaces for all positive-definite isounits. In fact, at the abstract, realization-free level, there is no difference between the conventional Minkowski space and the Minkowski-Santilli isospace, to such an extent that they can be expressed via the same symbols, only subjected to different interpretations. As we shall see, this feature has very important implications for numerous aspects of scientific knowledge.
Another property is that Santilli's isospaces unify all possible spaces with the same dimension. In fact, isoline element (2.16) clearly includes as particular cases the Minkowskian, Riemannian, Finslerian, non Desarguesian and other line elements. Hence, M*(r*, m*, E*) unifies all possible spacetimes in (3.1)-dimensions. In the event the positive-definiteness of the isounit is relaxed, M*(r*, m*, E*) unifies all possible 4-dimensional spaces, including the Euclidean one, the differentiation between one space and the otehr being set by the unit,
As we shall see, the above unification alone has far reaching implications, such as it has permitted the achievement of the first and only known, axiomatically consistent grand unification of electroweak and gravitational interactions that had escaped the best minds of the 20-th century, including Albert Einstein.
Santilli's geno- and hyper spaces have implications perhaps more intriguing those of the isospaces, because the former provide the first known geometric representation of irreversibility by embedding the direction of time in the geno- and hyper-metric itself, while the new spaces remain isomorphic to the original space even thogh, quite remarkably, the geno- and hyper-metrics are not necessarily symmetric.
Isospaces were first presented in two historical papers of 1983 on the structural generalization of the Minkowski space, the Lorentz symmetry and special relativity, with classical representation in the paper
Lie-isotopic lifting of special relativity
for extended deformable particles
R. M. Santilli, Lettere Nuovo Cimento Vol. 37, 545-555 (1983),
and operator counterpart
Lie-isotopic lifting of unitary symmetries and
of Wigner's theorem for extended deformable particles
R. M. Santilli, Lettere Nuovo Cimento Vol. 38, 509-521 (1983).
A more detailed mathematical treatment via the isotopies of the Euclidean space were presented in the two papers of 1985 quoted earlier
Lie-isotopic liftings of Lie symmetries, I: General considerations
R. M. Santilli,
Hadronic J. Vol. 8, 25-35 (1985)
Lie-isotopic liftings of Lie symmetries, II: Lifting of rotations
R. M. santilli,
Hadronic J. Vol. 8, 36-51 (1985)
In reality Santilli wrote first the latter two papers on the iso-Euclidean space and then wrote the paper on the isotopies of Minkowski space. Unfortunately the former ended up being published two years following the publication of the latter due to incredible editorial obstructions indicated elsewhere, of course, caused by novelty.
Iso-, geno- and hyper-spaces for matetr and their isoduals for antimatter were systematically p[resented in the historical memoir published by the rendiconti in 1996, with the initiation of their topology
Nonlocal-integral isotopies of differential calculus,
mechanics and geometries
R. M. Santilli, Rendiconti Circolo Matematico Palermo, Suppl. Vol. 42, 7-82 (1996).
Comprehensive studies were then published in Santilli's various books, including
,p>
"Elements of Hadronic Mechanics", Vol. I: "Mathematical Foundations"
R. M. Santilli, Ukraine Academy of Sciences (1993),
"Elements of Hadronic Mechanics"
Vol. II: "Theoretical Foundations"
R. M. Santilli, Ukraine Academy of Sciences (1994)
Systematic mathematical studies on the new spaces and the the resulting new topology were conducted in the following monograph among various others studies 9see the general bibliography)
Fundamentos de la Isoteoria de Lie-Santilli
Raul M. Falcon Ganfornina and Juan Nunez Valdes International Academic Press (2001)
2.5. DISCOVERY OF ISO-, GENO-, HYPER-SYMPLECTIC GEOMETRIES AND THEIR ISODUALS (1996)
As it is well known, the symplectic geometry provides one of the most rigorous studies for classical Hamiltonian systems, as well as for their quantization. Hence, Santilli could not escape a re-inspection of the symplectic geometry because his main physical objective was to represent the
most general possible (sufficiently smooth) non-Hamiltonian systems.
Consider the conventional canonical symplectic structure on a cotangent bundle with local charts r and p on the reals, ω = dp ∧ dr. It was easy for Santilli to formulate its isotopic covering on an isocotangent bundle with local chart r*, p* on the isoreals
(2.17) ω* = d* p* ∧ d* r*,
that, as one can see, coincides with the conventional two-form for all constant isounits, but possesses otherwise dramatic differences with the conventional version because it does allow the desired representation of all well behaved equations of motion with all possible potential and nonpotential forces.
These studies lead to what are today known as Santilli iso-, geno-, and hyper-symplectic geometries for matter and their isoduals for antimatter. Their most salient feature is that of coinciding with the conventional symplectic geometry at the abstract level to such an extent that Santilli insists in writing the equations for his covering geometries via the symbols of the conventional geometry, and merely subject them to a broader interpretation.
The above coverings of the symplectic geometry were first published in the monograph
"Elements of Hadronic Mechanics", Vol. I: "Mathematical Foundations"
R. M. Santilli, Ukraine Academy of Sciences (1993),
as well as in his mathematical memoir
Nonlocal-integral isotopies of differential calculus,
mechanics and geometries
R. M. Santilli, Rendiconti Circolo Matematico Palermo, Suppl. Vol. 42, 7-82 (1996).
2.6. UNIFICATION OF MINKOWSKIAN AND RIEMANNIAN GEOMETRIES (1998)
A very special feature of Santilli's isotopies is that of unifying seemingly different structures into a covering form that enjoys the basic property of invariance. Following the achievement in 1983 of his iso-Minkowski spaces (Section 2.4), Santilli realized that there is no difference between his iso-Minkowski metric m*(r, ...) and a conventional Riemannian metric g(r) since the explicit form of the characteristic quantities ni is unrestricted by the isotopies (only their positive-definite character is requested).
But Santilli knew at that time (early 1990s) that the iso-Minkowski spaces are isomorphic to the conventional space. Hence, his isotopic methods offered a unique possibility of unifying the Minkowskian and the Riemannian geometries, with far reaching implications, such as the first axiomatically consistent grand unification of electroweak and gravitational interactions previewed in the physics section.
In this way, Santilli achieved a new geometry on isospaces over isofields, today called Minkowski-Santilli isogeometry equipped with all the machinery of the Riemannian geometry (such as covariant derivative, Christoffel's symbols, etc.), that does unify the Minkowskian and Riemannian geometries, while admitting both as particular cases depending on the selected isounit.
This additional historical achievement was published by Santilli in various works, with primary presentation in the memoir>br>
Isominkowskian geometry for the gravitational treatment of matter
and its isodual for antimatter
R. M. Santilli, Intern. J. Modern Phys. D Vol. 7, 351-407 (1998).
Numerous papers then appeared showing the so called "direct universality" of the Minkowski-Santilli isogeometry, that is, the capability of admitting as particular cases all infinitely possible (non singular) geometries on a (3_1)-dimensional space (universality), directly in the selected coordinates and metric without any need for the transformation theory (direct universality). Among numerous papers in this aspect, we quote here the following
Universality of Santilli's iso-Minkowskian geometry
A. K. Aringazin and K. M. Aringazin, in "Frontiers of Fundamental Physics"
M. barone and F. Selleri, Editors, Plenum 91995)
2.7. ISOTOPIC COVERING OF LIE'S THEORY AND ITS ISODUAL (1978)
As it is well known, Lie's theory has been the fundamental mathematical tool of the 20-th century quantitative sciences, thus, having be the subject of vast attention and having achieved a vast diversifications into various branches, such as:
1) The universal enveloping associative algebra U over a field F(n, x, E) as a vector space whose element are: the unit matrix E = Diag. (1, 1, ..., 1) with the dimension of the selected representation; the N (Hermitean) generators Gk, k = 1, 2, 3, ..., N, with conventional associative products Gi x Gj; and the infinite-dimensional basis characterized by the Poincare'-Birkhoff-Witt theorem via the ordered monomials
(3.18) U: E, Gk, Gi x Gj i ≤ j, Gi x Gj x Gk i ≤ j &le k, ...
which basis is necessary for the definition of exponentiation W = exp (G x w x i), where w ε F, and other operations on U;
2) The N-dimensional Lie algebra L which is the antisymmetric algebra U- attached to U with Lie product and closure relations
(2.19) L: [Gi, Gj] = Gi x Gj - Gj x Gi = Cijk x Gk,
where the Cs are the structure constants of L;
3) The Lie group g whose realization most important in physics is that of Lie's the transformation groups of a quantity Q(w) that can be generically written in the following finite and related infinitesimal forms
(2.20) g: Q(w) = W(w) x Q(0) x W(w)† = exp (G x w x i) x Q(0) x exp( - i x w x G),
(2.21) i x dQ / dw = [Q, G] = Q x G - G x Q;
plus the representation theory generally constructed either on a right acting module u or, equivalently for Lie's theory, the left acting module -u,
It should be recalled that Lie's theory characterizes the fundamental dynamical equations of quantum mechanics, those of the time evolution via Eqs. (2.21) with w representing time t. Lie's theory also characterizes all fundamental symmetries in physics, such as the Lorentz and Poincare' symmetries at the foundation of special relativity, the SU(3) symmetry for the classification of particles, etc.
Immediately following the study of Lie's theory during his graduate studies in physics in Torino, Italy, in the late 1960s, Santilli realized the excessive limitations of the theory, since Lie's theory solely applies for systems that are linear, local-differential and Hamiltonian (canonical at the classical level and unitary at the operator level), while the systems of the real world are generally nonlinear, nonlocal-integral and admit forces both Hamiltonian and non-Hamiltonian interactions. Hence, Santilli set in the late 1960s his goal to reach a structural generalization of Lie's theory applicable to a broader class of systems.
Following decades of silent research, Santilli released in 1978 an isotopic (axiom-preserving) generalization (he called lifting) of each branches of Lie's theory, today known as the Lie-Santilli isotheory,, that constitutes one of the biggest mathematical and physical discoveries of the 20-th century, not only because of fundamental mathematical novelty, but also because of its predictable far reaching implications for all quantitative sciences.
Santilli's Lie-isotopic theory is based on all preceding mathematical discoveries, that is, its correct formulation requires isofields, isospaces, isodifferential calculus, isofunctional. analysis, etc., to such an extent that the lack of isotopic lifting of only one methodological aspect of Lie's theory causes catastrophic inconsistencies (lack of invariance of the theory under its own action, etc.). In fact, the mixing of Lie and Lie-Santilli's methods would be like formulating the conventional Lie's theory on Santilli's isofields, resulting in evident inconsistencies.
Under the above understanding, the presentation of Santilli's Lie-isotopic theory is now, following its discovery, rather elementary and its main branches can be summarily presented for the applied mathematicians as follows:
1*) The universal enveloping isoassociative algebra U* over an isofield F*(n*, x*, E*) as a vector space whose element are: the isounit E* = 1/T (where the positive-definiteness is assumed to preserve Lie's axioms and the dimension is that of the used isorepresentation); the same (Hermitean) generators Gk, k = 1, 2, 3, ..., N, of Lie's theory with isoassociative product and related isounit
(2.22) Gi x* Gj = Gi x T x Gj
(2.23) E* x* G* = G* x* E* = G* ∀ G ε U*
and the infinite dimensional isobasis characterized by the Poincare'-Birkhoff-Witt-Santilli isotheorem with ordered isomonomials
(2.24) U*: E*, Gk, Gi x* Gj i ≤ j, Gi x* Gj x* Gk i ≤ j &le k, ...
permitting the definition of isoexponentiation
(2.25) W*(w*) = E* + i* x* w* x* G/1 ! + ... = [exp(G x T x w x i)] x E* = E* x [exp(i x w x T x G)],
and other operations on U*;
2*) The N-dimensional Lie-Santilli isoalgebra L* which is the antisymmetric isoalgebra U*- attached to U* with Lie-Santilli isoproduct and closure relations
(2.26) L*: [Gi, Gj]* = Gi x* Gj - Gj x* Gi = Gi x T x Gj - Gj x T x Gi = Cij*k x* Gk,
where Cij*k characterizes the isostructure isofunctions of LCijk with constant particularizations;
3*) The Lie-Santilli isogroups g* whose realization most important in physics is that of Santilli's isotrasformation isogroups of a generic quantity Q*(w*) on U* over F* that can be written in the following finite and infinitesimal forms each in a dual way, the formulation on U* over F* and its projection on U over F
(2.27) g*: Q*(w*) = W*(w*) x* Q*(0*) x* W*(w*)† = exp (G xT x w x i) x Q(0) x exp( - i x w x T x G),
(2.28) i* x* d*Q* / d*w* = [Q, G]* = Q x T x G - G x T x Q;
plus the isorepresentation isotheory generally constructed either on a right acting isomodule u* or, equivalently, the left acting isomodule -u*.
As one can see, Santilli's isotheory causes the emergence of a generally nonlinear, nonlocal and non-Hamiltonian operator T in the exponent of the isotransformation laws, as well as in the broader isobrackets of the infinitesimal transforms, thus permitting indeed the originally desired extension of Lie's theory to nonlinear, nonlocal and non-Hamiltonian systems with far reaching implications indicated in the physics and other sections.
Remarkably, Santilli proved the "direct universality" of his isotheory for all well behaved nonlinear, nonlocal and non-Hamiltonian systems via an elegant theorem establishing that: All sufficiently smooth nonlinear, nonlocal-integral and non-Hamiltonian systems (noncanonical or nonunitary) on conventional spaces over a conventional field always admit an isounit for which their identical reformulations on isospaces over isofields are isolinear, isolocal and isocanonical (or isounitary, that is, verify the axioms of linearity, locality and Hamiltonian character on isospaces over isofields.
The reformulation is merely done by embedding all nonlinear, nonlocal and non-hamiltonian terms in the isounit.
This important property is the conceptual essence of Santilli's isotheory in both its mathematical meaning and physical applications. Because of its mathematical foundations, Lie's theory is strictly linear, local-differential and hamiltonian (canonical or unitary) on its conventional spaces over an ordinary field. In the event Santilli had not preserved at the abstract level these fundamental properties, his theory could not have possibly called an "isotopy" (axiom-preserving) lifting of Lie's theory. In turn, the physical departures would have been without scientific value, e.g., because of generalizations of special relativity and quantum mechanics that do not admit conventional theories as particular cases, impossibility to achieve a grand unification, etc.
Th axiomatic unity of the conventional Lie theory and its isotopic covering is such that Santilli insists in presenting the latter with the same symbols of the former, only subjected to a broader realization, as it is the case for isonumbers, isospaces, isogeometries, etc.
As we shall see, the above property also differentiates dramatically Santilli's studies from a variety of other attempts to generalize Lie's theory, all known today to verify the Theorems of Catastrophic Mathematical and Physical Inconsistencies recalled in Section 3, precisely because of the broadening of Lie's theory, on one side, combined with the preservation of the conventional mathematics, on the other side.
The above isotopic lifting of Lie's theory was constructed by Santilli for the the sole treatment of matter For the classical treatment of antimatter in such a way to achieve compatibility with the operator formulations via charge conjugation, Santilli needed an anti-isomorphic image of the above Lie-isotopic theory that he constructed via his isodual map (2.9) applied to the totality of quantities and their operations of the Lie-isotopic theory. This resulted in two new coverings of Lie's theory today known as Santilli isodual Lie theory and isodual Lie-isotopic theory, that is not reviewed here for brevity.
Santilli released the discovery of the isotopic covering of each branch of Lie's theory in 1978 when at Harvard University under DOE support in the two hundred pages historical memoir
On a possible Lie-admissible covering of Galilei's relativity
in Newtonian mechanics for nonconservative and Galilei form-noninvariant systems
R. M. Santilli, Hadronic J. Vol. 1, 223-423 (1978),
and expanded the theory in the series of volumes published by the most prestigious scientific house of the time, Springer Verlag, in its most prestigious series of Text and Monograph in Theoretical Physics
"Foundations of Theoretical Mechanics, I: The Inverse Problem in Newtonian Mechanics"
R. M. Santilli, Springer-Verlag (1978)
"Foundations of Theoretical Mechanics, II: Birkhoffian Generalization of hamiltonian Mechanics"
R. M. Santilli, Springer-Verlag (1982).
These original presentations were indeed based on isospaces, but defined on conventional fields. Subsequently, Santilli discovered the lack of completion of this formulation and, following the discovery of the isonumbers done specifically for that scope, reached a mathematically consistent formulation in various works, such as in the monograph that included a treatment of Santilli's isodual Lie theory and isodual Lie-isotopic theory
,p>
"Elements of Hadronic Mechanics", Vol. I: "Mathematical Foundations"
R. M. Santilli, Ukraine Academy of Sciences (1993),
"Elements of Hadronic Mechanics"
Vol. II: "Theoretical Foundations"
R. M. Santilli, Ukraine Academy of Sciences (1994)
A comprehensive presentation of the isodual Lie theory and the isodual Lie-isotopic theory is available in the monograph
"Isodual Theory of Antimatter, with Application to Antigravity, Grand Unification and Cosmology",
R. M. Santilli, Springer (2006)
A presentation also authored by Santilli dated 2008 is available in the monograph with a treatment of the Lie,m lie-isotopic theories and their isoduals
Hadronic Mathematics, Mechanics and Chemistry, III:
Iso-, Geno-, Hyper-Formulations for Matter
and Their Isoduals for Antimatter
R. M. Santilli, International Academic Press (2008)
Due to its historical importance, the Lie-Santilli isotheory has been the subject of numerous independent studies, among which we can quote the review papers
An introduction to the Lie-Santilli isotopic theory
J. V. Kadeisvili, Mathematical Methods in Applied Sciences Vol. 19, 1349-1395 (1996)
Foundations of the Lie-Santilli isotheory
J. V. Kadeisvili, Rendiconti Circolo Matematico Palermo, Suppl. Vol. 42, 83-135 (1996).
and the monographs
"Mathematical Foundation of the Lie-Santilli Theory"
D. S. Sourlas and G. T. Tsagas, Ukraine Academy of Sciences 91993).
"Santilli's Isotopies of Contemporary Algebras
Geometries and Relativities",br>
J. V. Kadeisvili, Ukraine Academy of Sciences, Second edition (1997)
Fundamentos de la Isoteoria de Lie-Santilli
Raul M. Falcon Ganfornina and Juan Nunez Valdes International Academic Press (2001)
For a comprehensive list of all controtbnutions on the Lie-santilli isotheory, the interested scholar is suggested to consult the General Bibliography.
2.8. LIE-ADMISSIBLE COVERING OF THE LIE-ISOTOPIC THEORY AND ITS ISODUAL (1967)
Again remarkably, Santilli remained dissatisfied with his own Lie-isotopic theory for physical and not mathematical reasons. Due to its structure and underlying topology, Lie's theory is ideally suited to represent a closed-isolated system of particles that, being necessarily abstracted as point-like, have no collisions, thus characterizing a Hamiltonian system (namely, a system entirely described by the Hamiltonian). This is typically is the case for the atomic structure and other systems. In these cases, the antisymmetric character of Lie's brackets [A, B] = A x B - B x A = - [B, A] permits the representation of the conservation of the total energy and other familiar total quantities (represented in physics by the generators G)
(2.29) i x dH/dt = [H, H] = H x H - H x H = 0.
Santilli's Lie-isotopic theory does enlarge the class of represented systems into particles that are expected (see Section 3), thus experiencing collisions with both Hamiltonian and non-Hamiltonian interactions, as it is the case at a classical level by the structure of a planet such as Jupiter, or a nucleus at the operator level. However, the systems remain closed-isolated as for the conventional Lie case because Santilli's isotopic product is also antisymmetric, [A, B]* = A x T x B - B x T x A = - [B, A]*, thus equally leading to the same total conservation laws characterized by Lie's theory,, such as
(2.30) i x dH/dt = [H, H]* = H x T x H - H x T x H = 0,
in which H is the conventional Hamiltonian and T represent all contact non-Hamiltonian interactions and effects (see Section 3).
Hence, the Lie-isotopic theory cannot be a final theory because the systems of the physical reality are, in general, open, nonconservative and irreversible, as it is the case for a constituent of Jupiter's atmosphere or a proton in the core of a star, when considering the rest of the system as external.
Santilli then searched for a covering of Lie's isotopic theory with a product (A, B) that is neither totally antisymmetry not totally symmetric, (A, B) ≠ ± (B, A) as a condition to characterize time-rate-of-variations f(t) of physical quantities,
(2.31) i x dH / dt = (H, H) = f(t) ≠ 0,
since conservation laws are a trivial particular case.
While doing his Ph. D. studies at the University of Torino,. Italy, in the late 1960s, Santilli conducted for years a comprehensive search at European mathematical libraries to identify the desired covering of Lie's theory. He was finally rewarded with the identification of a paper of 1947 by the American mathematician A. A. Albert who introduced, without any specific realization or elaboration, the notion of Lie-admissible algebras as a (generally nonassociative) algebra U with abstract elements a, b, c, ... and abstract (generally nonassociative) product ab such that the attached algebra U- given by the same vector space as U but equipped with the product [a, b] = ab - ba, is Lie.
Albert also introduced the notion of Jordan-admissible algebra as the same algebras U when such that the attached algebra U+ with product {a, b} = ab + ba is Jordan. Following additional extensive library search, Santilli could only identify in European mathematics libraries a second note in the field by M. Tomber, although without realizations or elaborations.
Armed with Albert's notion, Santilli published in 1967 the following paper on the embedding of Lie algebras in Lie-admissible algebras verifying central condition (2.31)
Embedding of Lie-algebras in nonassociative structures
R. M. Santilli, Nuovo Cimento Vol. 51, 570-576 (1967).
where he presented for the first time a specific realization of Lie-admissible and Jordan-admissible algebras with product (A, B) = p x A x B - q x B x A identified in more details in the physics section
To understand the novelty of this paper (and others by Santilli wrote in 1967-1968 not quoted here for brevity), we recall that in 1967 Santilli moved from the University of Torino, Italy, to the University of Miami, Coral Gables, Florida, for a one year stay. During that time, he applied for a job to virtually all Department of Physics in the U. S. A. by presenting with pride his discovery of Lie-admissible and Jordan-admissible algebras and their applications for the characterization of the time rate of variation of physical quantities. To his demise, no physicist in the U. S. A. knew the existence or meaning of these algebras.
Numerous applications for a job at various U. S. departments of mathematics turned out also to be sterile because of the general lack of knowledge by mathematicians of the time of the algebras herein considered. In fact, the above 1967 paper was the very first on Lie-admissible and Jordan-admissible algebras in the physic literature and it was the mere third paper in the field in the mathematics literature, including the two preceding papers by Albert and Tomber duly quoted in the above listed reference.
In this way, Santilli understood that there was no possibility to secure an academic job in the USA with so advanced a research. He then turned his attention to orthodox lines of research and soon got a position at Boston University. In fact, for about ten years Santilli published excellent but fully aligned papers at Phys. Rev. MIT Annals of Physics and orthodox journals of that nature.
It was only in 1978 that Santilli decided to return to his "first scientific love" and released his studies on Lie-admissibility in the historical 200 pages long memoir quoted in Section 2.7. He subsequently developed further these studies resulting in a covering of his Lie-isotopic theory today known as Santilli's Lie-admissible theory (or genotheory). that is based on the preceding discoveries of genofields, genospaces, genodifferential calculus, etc. and can be outlined via the following branches:
l1r) An enveloping genoassociative algebra Ur with ordered product to the right over the genofield to the right Fr(nr, xr, Er) with elements given by: the genounit to the right Er = 1/S; the generators Gk, k = 1, 2, ...,. N (as for the original Lie algebra), ordered genoassociative products to the right and related genounit
(32) Er = 1/S, Gi xr Gj = Gi x S x Gj,
(2.33) Er xr Gk = Gk xr Er = Gk ∀ Gk ε Ur;
the infinite-dimensional genobasis acting on a genomodule to the right ur
(2.34) Ur: Er, Gk, Gi xr Gj, i ≤ j Gi xr Gj xr Gk, i ≤ j ≤ k, , ....
and related genoexponentiation to the right
(2.35) Wr(wr) = Er + ir xr wr G/1! + ... = [exp(G x S x w x i)] x Er,
plus an enveloping genoassociative algebra to the left lU on the genofield to the left lF(ln, lx, lE) with elements: the genounit to the left lE = 1 / R; the generators kG (ordered to the left), k = 1, 2,..., N, with genoproduct and genounit
(2.36) lE = 1/R, iG lx jG = iG x S x jG,
(2.37) lE lx kG = kG lx lE = kG ∀ kG ε lU
the infinite dimensional genobasis acting on a genomodule to the left lu (where now ul ≠ ± lu)
(2.38) lU: lE, kG, iG lx jG, i ≤ j, iG lx jG lx kG, i ≤ j ≤k, ...
genoexponentiation to the left
(2.39) lW(lw) = lE x [ exp(i x w x R x G)],
and subsidiary condition
(2.40) lE = (Er)†,
important in physical applications, e.g., to connect consistently motions forward and backward in time. The combined action of the two genoenvelopes lU x Ur then act on the genobymodule lu x ur which is the representation genospace of the theory.
l2r) Santilli's Lie-admissible algebras lLr as the bimodular algebra attached to lU x Ur characterized by the new product and closure rules
(2.41) lLr: (iG, Gj) = iG lx jG - Gj xr Gi = Gi x R x Gj - Gj x S x Gi = lCrkij x Gk,
where the last expression is the projection of the algebra in the space of the original Lie algebra. As one can see, the resulting new product, here generically written (A, B) = A x R x B - B x S x A, is indeed jointly Lie-admissible and Jordan admissible although in Santilli's isotopic sense because
(2.42) [A, B]* = (A, B) - (B, A) = A x L x B - B x L x A, L = R + S,
(2.43) {A, B}* = (A, B) + (B, A) = A x J x B + B x J x A, J = R - S,
l3r) Santilli genotransformation groups lgr characterized by the left and right genoexponentiations (here written for simplicioty in the representation space of the original Lie algebra)
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(2.44) lgr: Wr xr Q(0) l lW = exp(G x S x t x i) x Q(0) x exp(-i x t x R x G).
with infinitesimal verison characterized precisely by Santilli Lie-admissible brackets in the following simplifieds form
(2.45) i x dQ/dw = (Q, G) = A x R x G - G x S x Q,
where G and w are the same generator and parameter as those of the attached Lie-isotopic algebra.
Quite remarkably, Santilli proved that his Lie-admissible covering of his Lie-isotopic theory is isomorphic to the Lie-isotopic and conventional Lie theory despite the lack of totally antisymmetric character of the product. This unexpected property was proven by noting that each of the two genoassociative algebras lU and Ur, when defined on the respective modules l and ur over the corresponding genofields lF and Fr are isomorphic to the conventional associative enveloping algebra U over F. The isomorphismnt hen follows between the Lie-admissible, Lie-isotopic and Lie theory under the use of the same generators and parameters and positive definite units.
The understanding of this important mathematical discovery, rather crucial for quantitative representation of irreversibility, can be seen by noting that, when the two products A x R x B and B x S x A are considered with respect to the conventional unit I of Lie's theory, the two algebras with products (A, B) = A x R x b - B x S x A and [A, B] = A x B - B x A are manifestly non-isomorphic.
When the product A x R x B is computed with respect to the genounit Er = 1/R, the result is equivalent to that of the product B x S x A represented with respect to the genounit lE = 1/S, and both products are equivalent to the product A x B with respect to the unit E = 1.
Santilli decomposed his Lie-admissible product into a totally antisymmetric and a totally symmetric forms,.
(2.46) (A, B) = [A, B]* + {A, B}* = (A x Y x B - B x Y A) + (A x Z x B + B x Z x A), R = Y + Z, S = Y - Z,
and proved the following important
THEOREM 2.1: The Lie-admissible algebras with product (A, B) are "directly universal," in the sense of admitting as particular cases all possible algebras on a field of characteristic zero as currently understood (universality) without use of the transformation theory (Direct universality).
In fact Santilli;i Lie-admissible algebras contain as particular cases all known or otherwise possible algebras with a bilinear composition law, such as: associative, flexible, alternative, Lie, Jordan, Lie-isotopic, Jordan-isotopic, supersymmetric and any possible other algebra.
The above presentation is solely intended for Santilli's Lie-admissible treatment of matter in irreversible conditions. For the corresponding treatment of antimatter we have Santilli's isodual Lie-admissible theory, that can be constructed via the application of the isodual map (2.9) to the totality of the quantities and their operation of the Lie-admissible theory.
Santilli presented his Lie-admissible covering of his Lie-isotopic theory in the historical 200 pages long memoir quoted above
On a possible Lie-admissible covering of Galilei's relativity
in Newtonian mechanics for nonconservative and Galilei form-noninvariant systems
R. M. Santilli, Hadronic J. Vol. 1, 223-423 (1978)
and presented its physical application in the joint memoir submitting hadronic mechanics as a covering of quantum mechanics with his lie-admissible structure
Need of subjecting to an experimental verification the validity within a hadron of Einstein special relativity and Pauli exclusion principle
R. M. Santilli, Hadronic J. Vol. 1, 574-901 (1978)
he then developed further his lie-admissible theory in the two volumes
"Lie-Admissible Approach to the Hadronic Structure, I: Non applicability of the Galilei and Einstein Relativities,"
R. M. Santilli, Hadronic Press (1978)
Lie-Admissible Approach to the Hadronic Structure, II: Coverings of the Galilei and Einstein Relativities"
R. M. Santilli, Hadronic Press (1982)
Additional presentations were made by Santilli in the two monographs published by Springer-Verlag in 1978 and 1982; a recent update is available in the 2008 monograph
"Foundations of Theoretical Mechanics, I: The Inverse Problem in Newtonian Mechanics"
R. M. Santilli, Springer-Verlag (1978)
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"Foundations of Theoretical Mechanics, II: Birkhoffian Generalization of hamiltonian Mechanics"
R. M. Santilli, Springer-Verlag (1982).
Subsequently, he developed his Lie-admissible theory and its isodual in the two monographs
"Elements of Hadronic Mechanics", Vol. I: "Mathematical Foundations"
R. M. Santilli, Ukraine Academy of Sciences (1993),
"Elements of Hadronic Mechanics"
Vol. II: "Theoretical Foundations"
R. M. Santilli, Ukraine Academy of Sciences (1994)
A more recent presentation is available in the monograph
Hadronic Mathematics, Mechanics and Chemistry, Vol. III: Iso-, Geno-, Hyper-Formulations for Matter
and Their Isoduals for Antimatter
R. M. santilli, International Academic Press (2008),
and the memoir published by the Italian Physical Societ,y where Santilli applies his Lie-admissible theory for the first and only known invariant representation of irreversibility for matter and, separately, for antimatter, originating at the most elementary level of nature, that of elementary particles and antiparticles
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Lie-admissible invariant representation of irreversibility for matter and antimatter at the classical and operator level
R. M. Santilli, Nuovo Cimento B Vol. 121, p. 443-595 (2006)
Numerous mathematical works on lie-admissibility can be located in the General Bibliography.
2.9. INTEGRABILITY CONDITIONS FOR THE EXISTENCE OF A LAGRANGIAN
2.9A. Integrability conditions in Newtonian mechanics (1978).
Virtually the entire scientific production of the 20-th century was based on the use of Lagrangian or Hamiltonian representations of Newtonian systems, then extended to operator formulations. Beginning with his graduate studies, Santilli set himself up to broaden these representations so as to avoid excessive abstractions and simplifications of reality, since said representations apply for point-like approximation of particles with sole action-at-a-distance interactions.
Hence, as part of his program, Santilli conducted a comprehensive study of the broadest possible systems representable via a Lagrangian or a Hamiltonian, and conducted this study via a systematic analysis of the integrability conditions for the existence of a Lagrangian or a Hamiltonian for given dynamical systems, calledconditions of variational selfadjointness.
By indicating with the symbol SA (NSA) forces or equations verifying (violating) the conditions of variational selfadjointness, Santilli writes Newton's equations in a form decomposing forces into a component derivable from a potential (SA) and a second term representing all forces not derivable from a potential )(NSA)
(2.47) m x dv/dt - FSA(r, v) - FNSA(t, r, v, ...) = 0.
and writes Hamilton's equations (1.2) in the corresponding form
(2.48) ( dr/dt - &part H(r, p)/&part p )SA = 0,
(2.49) [ (dp/dt + ∂ H(r, p)/∂ r )SA - F(t, r, p, ...) ]NSA = 0.
As we shall see in Section 3, Santilli's mathematics allows the reformulation of Newton's equation into an identical selfadjoint form merely formulated on generalized spaces over generalized fields. The regaining of selfadjointness permits the recovering an action function with consequential means for a rigorous map to contact non-Hamiltonian interactions into operator forms, with endless applications.
These studies resulted in the two monographs indicated earlier publisher by Springer-Verlag, written when he was at Harvard University, with the most comprehensive references in the field up to 1982 that required Santilli one full year of search in the Cantabridgean libraries (an impeccable ethical conduct that is per se a great rarity in the contemporary widespread plagiarisms in science),
"Foundations of Theoretical Mechanics, I: The Inverse Problem in Newtonian Mechanics"
R. M. Santilli, Springer-Verlag (1978)
"Foundations of Theoretical Mechanics, II: Birkhoffian Generalization of hamiltonian Mechanics"
R. M. Santilli, Springer-Verlag (1982).
2.9B. Integrability conditions in field theory (1975)
As indicated earlier, Santilli conceived first in 1967 his Lie-admissible theory and then studied its Lie-isotopic particularization. He did the same for the conditions of variational selfadjointness. In fact, when he was at the Center for Theoretical Physics of the Massachusetts Institute of Technology in the mid 1970s, Santilli first studied the integrability conditions for the existence of a Lagrangian or a Hamiltonian for the most general possible tensorial field equations, and published their simplification for Newtonian systems reviewed above when subsequently he was a Harvard University.
These studies produces the following three memoirs that constitute the most serious scholar works in the field ands remain grossly unsurpassed to this day in their essential results and mathematical rigor
Necessary and sufficient conditions for the existence of
a Lagrangian in field theory, I: Variational approach to
selfadjointness for tensorial field equations
R. M. Santilli, (MIT) Ann. Phys. Vol. 103, 354-408 (1977)
Necessary and sufficient conditions for the existence of
a Lagrangian in field theory, II: Direct analytic representation of tensorial field equations
R. M. Santilli, (MIT) Ann. Phys. Vol. 103, 409-468 (1977)
Necessary and sufficient conditions for the existence of
a Lagrangian in field theory, III: Generalized analytic representations of tensorial field equations
R. M. Santilli, (MIT) Ann. Phys. Vol. 105, 227-258 (1978)
3. SANTILLI'S DISCOVERIES IN PHYSICS
3.1. FOREWORD
In this section we outline the most important discoveries by Santilli in physics and provide copies of the original papers in free pdf downloads. As it was the acse for Section 2, we regret not to be able to outline subsequent contributions by independent researchers to avoid a prohibitive length, but they can be located in the General Bibliography on Santilli Discoveries
The serious scholar is suggested not to restrict the attention solely on individual topics, but provide primary attention to the overall mathematical and physical consistency as well as beauty of the entire scientific edifice.
None of the discoveries presented in this section has been disproved in the scientific literature to our best knowledge. Scholars are requested to inform the Foundation of the existence of papers in the refereed journal disproving any of the discoveries listed in this section for their outline, quotation and
listing in the related section.
During the first subsections, we shall use for clarity the conventional associative multiplication AB of numbers, vector fields, operators, etc., and use the symbol AxB for the same multiplication when initiating the presentation of classical or operator generalized theories.
3.2. ETHER AS A UNIVERSAL SUBSTRATUM (1952-1955)
Santilli was fascinated by the ether (or aether or space) since his high school studies in the 1950s he conducted in the city of Agnone, province of Isernia, Italy. A controversy was raging at that time on space conceived as a universal medium (or substratum) because such as conception was believed to be in conflict with special relativity due to its foundation on the lack of existence of a privileged reference frame.
An argument used to deny the existence of pace as a universal medium was the lack of "aethereal wind," namely, the absence of any resistance by Earth in its motion in space. Another argument was the use of Einstein's photon for the reduction of light to particles, thus eliminating the need for a medium to propagate electromagnetic waves.
In his first writings dating back to his school years, Santilli opposed these views. To begin, he saw no conflict between the existence of a universal medium and special relativity because, assuming that an absolute reference frame can be set at rest with said universal medium, that frame cannot be identified by man precisely in view of the relativity of motion.
In 1952, when 16 years old, Santilli delivered a seminar on Albert Einstein to the teachers and students of his high school whose transcript (in Italian) has been retrieved by our Foundation from the high school documents and made available in free pdf download:
"Albert Einstein"
Seminar delivered by R. M. Santilli in 1952 at the High School in Agnone, (Isernia), Italy,
Next, Santilli accepted the reduction of light to photons, but only for high frequencies, such as for UV or gamma rays, and rejected the reduction to photon for electromagnetic waves at large, such as those with large wavelength (e.g., radiowaves), thus considering the notion of [photon as an approximation of reality motivated by the characteristics of electromagnetic waves to cause an impulse when hitting a surface. As a general position, he writes (in Italian): My voice can be heard because there is air as a medium propagating sound waves and, in the absence of air, no voice can be propagated. By the same token, my face can be seen because there is a universal medium to propagate light and, again, in the absence of a universal medium, light could not exist or propagate.
By nothing that sound waves are longitudinal because the medium (air) is compressible, and by noting that electromagnetic waves are transversal, Santilli assumed that space is a universal medium with very high rigidity and, consequently, very high energy density (otherwise light would be characterized by longitudinal or other forms of waves).
Finally, Santilli dismissed the hypothesis of the "aethereal wind" because he conceived space as the universal substratum necessary for the characterization not only of electromagnetic waves but also of the elementary particles constituting matter, the difference being that oscillations of space propagate in the former case in the form of waves, while they are stationary in the latter (unless moved).
In particular, Santilli assumed the electron to be a pure oscillation of space, that is, the oscillation of a point of space without any oscillation of a "little mass" or any other material entity, and assumed the same for all other particles constituting matter, although with a much more complex oscillating structure.
In this way, Santilli eliminates the "aethereal wind" by writing: Contrary to our sensory perception, space is completely full of the universal medium, while matter is completely empty, in the sense that, following the reduction of matter to the structure of elementary particles, we have pure oscillatory energy of space without any matter component as perceived by us.
Consequently, when we move an object, we move no material substance as perceived by us, and we merely transfer the oscillations constituting matter from one region of space to another, without any possibility for the "aethereal wind" to exist. hence, inertia is a natural resistance by space against changes of steady propagation of the characteristic oscillations of a given body.
As we shall see, Santilli returned to his conception of space some 50 years later following the discovery of new mathematics permitting quantitative studies of the expected interconnection between space as a universal medium with high energy density and matter (achieved via the isotopies of Hilbert spaces and fields at the foundation of hadronic mechanics), In particular, his conception of space emerged rather forcefully in his studies on the synthesis of the neutron and the expected continuous creation in our universe, alternatives to the neutrino conjecture via longitudinal impulses propagating through space, geometric propulsions with unlimited speeds without fuel tanks, and other far reaching conceptions.
Our Foundation has identified some (but not all) initial writings by Santilli and we make them here available as free pdf downloads for interested scholars. We list the first book written by Santilli in 1955 (but not listed in his CV) and two articles of 1955 and 1956. Note the title of the second article (Elimination of the mass in atomic physics) that anticipate the need to replace the mass with energy in newton's and Einstein's gravitation discovered years later and outlined below.
"Principi su una Teoria Unificata sulla Fisica Atomica" (Principles for a Unified Theory in Atomic Physics)
R. M. Santilli,
Naples (1955)
"Eliminazione della massa nella fisica atomica" (Elimination of mass in atomic physics),
R. M. Santilli, Phoenix, Volume 1, pages 222-227 (1955)
Perche' lo spazio e' rigido (Why space is rigid)
R. M. Santilli,
Il Pungolo verde, Campobasso, Italy, (1956)
The Foundation is interested in providing financial support to studies on the ether as a universal substratum, under the conditions that the assumed characteristics of the ether allow a quantitatiove representation of the transversal character of light, as done by Santilli with his rigidity equivalence of the ether, thus excluding models of the ether as being a fluid and the like.
3.3. ORIGIN OF THE ELECTRIC AND MAGNETIC FIELDS (1955-1957)
As a natural continuation of the preceding conception of space, Santilli concentrated his attention in the structure of the electron as part of his 1957 thesis for the degree in physics at the University of Naples, Italy.
Starting from the compelling need for space to be a universal medium with high rigidity to characterize light via transversal waves, and the consequential need for the electron to be a pure oscillation of space in the sense indicated above, Santilli addressed the problem of the origin of the elementary charge and magnetic field or, equivalently, the structure of the electron.
His main intuition is that the electron is widely represented with its well known characteristic frequency
(3.1) ν = ω/2π = m c2 / h = 0.829 x 1020 Hz.
Hence, he argued that the elementary charge "e" cannot possibly be a constant as believed during the 20-th century, but must also show some form of periodic time dependence. The understanding is that a collection of elementary charges q = ∑k ek is indeed expected to be constant as per known experimental evidence.
The issue raised by the characteristic freqyency (3,1) is the following: If space is a universal medium with high rigidity, the oscillation of one of its points will propagate an oscillating force in the medium that can be safely assumed to decay with the inverse square of the distance. However, when such a force encounters another electron, the latter should oscillate, rather than being repelled.
The solution identified by Santilli is that the coupling of identical elementary charges activates only the repulsive part of the oscillating force, while the coupling of opposing charges activates only the attractive component of the oscillating force propagating through space.
Santilli then concluded with the hypothesis thatThe repulsive force between two identical electrons is not constant, but has the shape of half a sinusoid with the characteristic frequency of the electron. It should be indicated again that the above hypothesis solely applies for two electrons because, when considering a large number of electrons, the above periodicity is evident;ly averaged out, resulting into a constant force.
Hence, Santilli assumed that such an oscillation transfers to space an oscillating force with the same frequency, resunting in the followinving structure model of the elementary electric charge
(3.2) e = ± (2 h ν R )1/2 sin ωt,
In this way Santilli reached in 1957 a structural generalization of the Coulomb law for two elementary charges into a time dependent, pulsating form that, for the simplest possible case of two one-dimensional oscillations along the same axis can be written
(3.3) F = ± e2 / r2 = (2 h ν R/ r2) sin2 ω t,
where the positive (negative) sign denotes repulsion (attraction) and R is the amplitude of the oscillation, with much more complex expressions for oscillations in two and three dimensions (see for details the literature quoted below).
The conception of the electron as a pure oscillation of space is far from being trivia and should be taken seriously by researchers in the field, if nothing else, because alternatiuve hypotheses appears to lack plausibility. In fact, the addition of rotation to the pure oscillation of space creates a rosetta-type planar distribution with an SO(2) symmetry that (unlike the SO(3) case) admits angular momentum 1/2 as th lowest non-null state, thus allowing a structure model oid the electron spin.
Additionally, an oscillation of a point of a rigid medium propagates two different impulses in the medium, the radial one identified with the origin of the electric charge, and the trasversal one that propagates in the two directions opposite to the oscillation thys hjaving all pre-requisites for their interporetation as the origin of the elementary magnetic dipole moment, as illustrated in the figure.
Half a century has passed since these pioneering studies and, in view of the obscurantism created by Einstreinian theories, studies on space as a unievrsal substratum have been vastly ignored by the so-caleld "mainstream" of physics researcjh, with tbe consequential dismissal of studies on the origin of the electromagnetic field in favor of its description.
Yet, Santilli must be credited to have voiced a restorfation of serious scientific democracy with the addressing of truly fundamental physical issues irrespective of their political implications, a pattern that has been at the basis of Santilli's entire life.
Our Foundation has retrived Santilli's thesis (in Italian) at the University of Naples on the structure of the electron and the origin of its electromagnetic field, and makes it available in free pdf download:
"Fondamen ti per una teoria unbificata sulla struttura dell'elettrone" (Foundations for a unified theory on the structure of the electron)
R. M. Santilli,
Department of Nuclear Physics. University of Naples (1958)
Ethical notesz
In the 1970s, when in the USA, Santilli returned to these early study and he submitetd a paper to Physical Review Letters on the structure of hypotheses (3.2) and (3.3), essentially a review of his 1957 thesis, with a specific proposal for their experimental verification or denial via resonating mechanisms.
Unfortunately for science, Santilli received a very disacouraging response based on theoretical theologies, while he was suggesting the conduction of experiments for the verification or denial of the constancy of the electrostatic force between two electrons down to the characteristics frequency (3.1).
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Consequently, he abandoned the research, kept his studies for himself, and only in 1983 he released two short rview papers for publication in the Hadronic Journal and in Nuovo Cimento Letters merely to have a (generally ignored) record of his studies
A structure model of the elementary charge
R. M. Santilli, Hadronic J. Vol. 4, 770-784 (1981)
A conceivable lattice structure of the Coulomb law>br>
R. M. Santilli, Lettere Nuovo Cimento Vol. 37, 505-508 (1983)
The connection between Santilli's conception of the electron and the string theories appeared some half a century later should be noted. Unfortunately, the latter have been patterned along a priory political requirements, that of verifying special relativity. In fact, string theories are an attempt to formulate the extended character of particles in a way compatible with Einsteinian doctrines (since the latter solely admit point-particles as indicated earlier).
In any case, string theories are like an edifice in air without foundations due to the lack of general identification of the truly fundamenmtal notion, theentity that vibrates thus permitting the existence of rthe strings, since the universal substratum would be perceived as violating special relativity. Additionally, string theories in their current formulation verify the Theorems of Catastrophic Mathematical and Physical Inconsistencies of Noncanonicalk and Nonunitary Theories reviewed later on. Due to the excessive political foundations, as well as catastrophic inconsistencies technically identified below, string theories will be ignored.
The Foundation wan ts to be on record that the denial by Phys. Rev. Letters of a call to the experimental verification of laws (3.2) and (3.3) is a case of clear scientific obscurantism because hypotheses of such a magnitude for human knlowledge as laws (3.2) and (3.3) are, must be resolved experimentally, and their dismissal via theoretical theologies is a mere action for personal academic or other advantages.
The Foundation is interested in providing financial support for the experimental verification or denial of Santilli's laws (3.2) and (3.3) and is seeking interested experts in the field.
3.4. ORIGIN OF THE GRAVITATIONAL FIELD (1974)
Following the above pioneering studies on th structure of space and the origin of the electromagnetic field, it was natural for Santilli to study the origin of the gravitational field. This study was conducted in the 1970s when he was at the Center for Theoretical Physics of the Massachusetts Institute of technology.
Santilli initiated the study with the origin of the exterior gravitational field of the most elementary particle, the electron, whose mass is well known to be of entirely of electromagnetic origin. Hence, he reached the conclusion that the gravitational field of an electron is entirely of electromagnetic origin, and write the gravitational field equations on a Riemannian space in the form
(3.4) Rμ ν + gμ ν R = k Tμ ν,
where T is the energy-momentum tensor of the electromagnetic field of the electron and k is a constant.
Next, Santilli studied the exterior gravitational field of the πo particle as a bound state of one charged constituents called "parton" and its antiparticle (assumed to have the same elementary structure of the electron) in very high rotation at 1 fm mutual distance. By using the most advanced relativistic calculations, he discovered that the mass of the πo can also be of entire electromagnetic origin. Therefore, for the gravitational field of the πo Santilli also wrote the field equation in the form (3.1), namely, with a first order source tensor in the r.h.s.
He then passed to the study of ordinary massive bodies and reached the conclusion that the exterior gravitational field in vacuum of an ordinary massive body, whether charged or not, is entirely generated by the sum of the electromagnetic fields of all elementary constituents of the body considered, with field equations of type (3.4) having a source tensor in the r.h.s. of first order in magnitude (*that is not ignorable in first approximation) irrespective of whether the body considered is neutral or charged and with or without a magnetic field. In this case, Santilli characterized the source tensor T as the sum of a very large number of individual contributions and provided methods for its average.
He then passed to the problem of the origin of the interior gravitational field by recalling that, from a structural viewpoint, the main difference between the exterior and the interior problem is the additional presence in the interior case of short range, weak and strong interactions. Hence, for the interior gravitational problem of the πo particle, he wrote the field equations in the form
(3.5) Rμ ν + gμ ν R = k Tμ ν + w Wμ ν,
where Wμ ν is the energy-momentum tensor due to weak and strong interactions in the interior of the πo and w is another constant.
Santilli also noted that: the tensor Tμ ν is traceless, while the tensor Wμ ν is not; the source tensor of the interior problem gas a bigger numerical value of that for the exterior problem; and, consequently, he concluded that the inertial mass is bigger than the gravitational one, the former (latter) being characterized by the interior (exterior) problems.
Santilli then compared the above results (reached via first principles of classical and quantum electrodynamics) with Einstein's conception of the exterior gravitational; problem that, as well known, is based on its entire reduction to curvature without any source for neutral bodies, and celebrated field equations
(3.6) Rμ ν + gμ ν R = 0.
From the evident differences between Eqs. (3.1) or (3.5) and (3.6), Santilli concluded that: Einstein conception of gravitation as pure curvature is irreconcilably incompatible with classical and quantum electrodynamics because,
A) Either one assumes Einstein gravitation as being correct, in which case classical and quantum electrodynamics have to be profoundly reformulated in such a way to avoid a first order electromagnetic contribution contribution to masses:
B) Or one assumes classical and quantum electrodynamics as being valid, in which case Einstein's reduction of gravity to pure curvature without source (for the case of neutral bodies) must be abandoned.
Santilli then concluded the study of 1974 with its evidence consequence: The electromagnetic origin of the gravitational fields implies their "identification," thus eliminating the need for their "unification", with the understanding that the former (latter) field is described by second-order (first-order) equations.
In the late 1990s, he added the proof that Einstein's field equations for a neutral body are additionally incompatible with the Feud identity of the Riemannian geometry, since the latter requires two source tensors in the r.h.s of the field equations., one traceless and the other with trace, exactly as predicted by Santilli's origin of the gravitational field, Eqs. (3.2), plus various inconsistency theorems reviewed later on in this section.
The origin of the gravitational field and its identification with the electromagnetic field were published by Santilli in the paper:
Partons and gravitation: some puzzling questions
R. M. Santilli,
(MIT) Annals of Physics Vol. 13, 108-157 (1974)
The violation by Einstein's gravitation of the Freud identity of the Riemannian geometry and nine inconsistency theorems were presented in paper
Nine theorems of catastrophic inconsistencies of general relativity and their possible resolution via isogravitation
Ruggero Maria Santilli
Galilean Electrodynamics, Summer 2006, p. 43-79
with a general review in the volume
Hadronic Mathematics, Mechanics and Chemistry, Volume I: Limitations of Einstein's Special and General Relativities,
Quantum Mechanics and Quantum Chemistry
R. M. Santilli, International Academic Press (2008)
Ethical notes
The serious scholar should be alerted that Einstein's gravitation is one of the least scientific fields of inquiry because populated by Einstein's fanatics without any regard to scientific knowledge, solely intent in serving organized interests on Einsteinian doctrines. Any expectation of any serious scientific process under these conditions, even at seemingly "high ranking" scientific conduits, would be illusory.
We merely mention here the existence in the literature of a number of manipulations of Santilli's exterior identification of the gravitational and electromagnetic field evidently intended to preserve preferred theories in disregard of physical evidence. The most frequent manipulation is the claim that "Einstein's field equations do include a source tensor of electromagnetic origin in the r.h.s." which statement is correct but fraudulent on various counts, particularly when proffered by experts, because:
1) Santilli's origin of the gravitational field requires a source tensor that is of first order in magnitude for bodies with null electric and magnetic fields, in which case Einstein's field equations have no source at all;
2) Even assuming the case of a charged massive body, Einstein's equations solely admit a source tensor for the total electromagnetic field that is very small and of the order of 10-40 weaker than the gravitational field, thus ignorable for quantitative study, while Santilli's source tensor is that of the gravitational field, thus not being ignorable;
3) Assuming that the extremely weak source tensor in Einstein's field equations is acceptable (which is not the case because in conflict with quantum electrodynamics), the equation violate the Freud identity of the Riemannian geometry, since the latter require two first order source tensors with the structure of Santilli's equations (3.2)
Ths Foundation warns authors, editors and publishers against plagiarisms of Santilli's exterior identification of gravitation and electromagnetic interactions without a quotation of his paper of 1974 in th proper chronological order.
3.5. SYMMETRY OF THE ETHER (1970)
As indicated earlier, Santilli considers ether (or space) to be a universal substratum for all visible events in the universe, thus being the most fundamental and final frontiers of scientific knowledge. The physics community of the 20-th century did not accept this notion because it implies an absolute reference frame that is prohibited by special relativity, thus adapting nature to a preferred theory.
Being a physicist interested in quantitative studies, it was then natural for Santilli to search for the symmetry of the ether, that is, the spacetime symmetry admitting indeed a universal substratum for all visible events, while, of course, being compatible with available experimental evidence. The absence of such a symmetry originates from the fact that , there is no possibility to characterize sad notion of the ether via the fundamental spacetime symmetry of the 20-th century, the 10-dimensional Poincare' symmetry, here indicated in its simpler connected form
(3.7) P(3.10) = SO6(3.1) ⊗ T4,
where: SO6(3.1 represents the connected 6-dimensional Lorentz symmetry; T4 is the group of translations in Minkowski spacetime; and ⊗ is the semidirect product.
Hence, Santilli searched for a broadening of the Poincare' symmetry in such a way to admit special relativity as a particular case, while allowing means for the characterization of the ether via a primitive, spacetime symmetry.
The solution came in a series of papers written from 1970 on by Santilli in collaboration with the Jewish physicists P. Roman and J. J. Aghassi at the Department of Physics of Boston University. The proposal consisted in the 15-dimensional ether symmetry as called privately by Santilli and officially called in the publications the relativistic Galilei group G5 where 5 denotes the extension of the 4-dimensional Minkowski spacetime with coordinates xμ, μ = 1, 2, 3, 4, with an additional scalar u characterizing the ether as a universal medium, e.g., u representing the ether proper time. The new symmetry is characterized by the transformations
(3.8) Lorentz transformations xμ → Λνμ xν,
(3.9) Spacetime translations xμ → xμ + aμ,
(3.10) Spacetime boosts xμ → xμ + bμu,
with group structure
(3.12) G5 = {SO6(3.1) ⊗ T4(a)} ⊗ {T4(b) x T1(σ)},
and and generators of the Lie algebra
(3.13) g5 = {Jμν, Pμ, Xμ, E},
where: Jμν and Pμ are the conventional generators of the Poincare' algebra; Xμ is a position operator, and E is a energy operator, the latter two operators being a novelty of the new symmetry since they are impossible for the Poincare' symmetry. For additional technical data, interested readers are suggested to consult the literature below.
In summary, the Poincare' symmetry can be extended broadening into the ether symmetry (or the relativistic Galilei symmetry) G5 that admits as a subgroup both the Poincare' symmetry and the conventional (nonrelativistic) Galilei symmetry, as well as fundamental new features that are impossible in the Poincare' symmetry, such as the position and energy operators, a universal constant (originating from the scalar extension) and other intriguing features,
The use of the ether symmetry is then the following. The poincare' component is used for the representation of all data connected to special relativity with no change, including the adoption of all its experimental verifications. The remaining components mainly represent the interplay between cosmological aspects, the universal medium, and the event considered, that include the emergence of position and energy operators that are an evident consequence of the introduction of the proper time of the ether, u.
Needless to say, it would be presumptuous to claim that the ether symmetry is the correct spacetime symmetry for relativistic dynamics, and the same holds for the believe of the Poincare' symmetry as the final spacetime symmetry to the end of time. Yet, it is the opinion of the Foundation that, until experimental evidence disproving the new symmetry is identified, the ether symmetry is superior to the Poincare' symmetry, if nothing else, because of the much broader conception.
The 1970 paper below is the historical paper presenting the new spacetime symmetry. For numerous additional papers, particularly those on the representation theory and applications, interested scholars are suggested to consult Santilli curriculum.
A new dynamical group for the relativistic quantum
mechanics of elementary particles
A. Aghassi, P. Roman and R. M. Santilli,
Phys. Rev. D vol. 1, 2753-2765 (1970)
Ethical notes
The reader should be aware that the American Physical Society prohibited any mention of the intended use of the relativistic Galilei symmetry for the characterization of a universal substratum, for the evident political reason to avoid the perception of the paper being incompatible with Einsteinian doctrines. The presentation of the new symmetry adopted above has been derived by the Foundation from Santilli's unpublished manuscripts of the time, and coincides with the above quoted Phys. Rev paper only in the formulae.
Following the appearance of the proposal to replace the Poincare' symmetry with a broader spacetime symmetry, and the expected consequential broadening of special relativity, Santilli experienced unprecedented academic obstructions for the continuation of its study. For instance, Santilli was denied the "libera docenza" (an Italian governmental title of professor) at its last session held in Rome, Italy, by a committee headed by the Italian physicists V. De Alfaro of the University of Torino, R. Gattpo of the Univrsity of Geneva, Switzerland, and P. Budini (later changed into Budinovitch) of the ICTP, Trieste, Italy.
This denial was quite damaging to the credibility of the Italian physics community since the "libera docenza" was granted to all other applicants, even though Santilli had substantially superior publications (besides the new symmetry here presented, Santilli had numerous publications on Lie-admissible theories, the extension of the PCT theorem of the next section and numerous other listed in his curriculum), besides being the only candidate with the official position of Associate Professor at a U. S. university.
in view of these and other hardly credible academic obstructions, blatantly intended to maintain the dominance of Einsteinian doctrines via the suppression of scientific process on structural advances, Santilli abandoned the research in the field by stating: I believe that there is no possibility at this moment of due scientific process in surpassing Einsteinian theories due to excessive opposing interests with capillary organization on a world wide basis. I write papers beyond Einstein primarily for posterity because, unlike other fields, corrections in quantitative science are only a matter of time.
3.6. QFT (AND QCD) LIMITS FROM DISCRETE SYMMETRY VIOLATIONS (1974)
The rigorous implementatio of Lie's theory demands that the fundamental symmetry of special relativity, the Poincare' symmetry, is given by a continuous component characterized by the (connected) Lorebtz symmetry, and a discrete components characterized by space and and time inversions.
In the early part of the 20-th century, the entire Poincare' symmetry was assumed to be valid throughout the universe. The discovery of parity violation by weak iunteractions, rather than causing scientific joy, caused panic among the Einsteinian followers because of fear that the entire edifice may collapse. Interests on a world wide basis were then organized in the physics community to reach a vast consensus, intentionally without any technical examination, that "the violation of discrete symmetrries does not cause the violation of the continuous component of thge Lorentz symmetry or of special relativity," a popular political belief without scientific process that is still widespread nowadays.
Thanks ti his notorious independence of thought from popular, academic beliefs, Santilli conducted in the 1970s quantitative technical studies as to whether the violation of discrete symmetries implies that of the Lorentz symmetry and, consequently, of special relativity. The analysis was conducted with the most advanced and rigorous technical knowledge in quantum field theory of the time, that via Wightman's axioms.
Being an applied mathematcians, Sanbtilli was fascinated by the beauty of quantum field theory (QFT) characterized by Whitman axisoms. However, being a physicist, he also knew that such a theory had to admit limits of exact applicability. Thus, he initiated comprehesnive studies for the identification of such limits of applicability as a necessary foundation for suitable covering theories. The reader should be aware that these studies are of extreme complexity and, therecore, can be only reviewed here in their main conceptual lines.
The discrete symmetries of quantum field theories are given bythe following operations and their combinations:
(3.14) P (space inversion), C (charge conjugation), T (time inversion), PC, CT, PT, PCT.
The PCT theorem within the context of the vacuum expectation values (VEV) under the Wightman axioms essentially related the PCT conditions to the weal local commutativity conditions (WLC) under the assumption of Lorentz invariance SO(3.1) for the vacuum expectation values as well as the (quantum vecuum), boundedness of the energy from below and other conditions permitting smooth analytic continuations.
While supervising a Ph. D. thesis of one of his students, the Greek physicist C. N.Ktorides, Santilli achieved the extension of the PCT theorems to all discrete spacetime symmetries, a possibility simply unknown at that time. To achieve this goal, he derived the following dual discrete symmetries
:
(3.15) P# = (PC)(WLC), C# = WLC, T# = (TC)(WLC), PC# = P(WLC), CT# = T(WLC), PT# = (PCT)(WLC), PCT# = PT(WLC).
We then have the following:
THEOREM 3.6A: Under Lorentz invariance, analyticity and energy bound3dness from below, the validity (at a Jost point) of any discrete symmetry in a quantum field theory satisfying the Whitman axioms implies that of its duel and vice versa:
(3.16) P ↔ T#, C ↔ PCT#, T ↔ P#, PC ↔ CT#, CT ↔ PC#, PT ↔ C(WLC), PCT ↔ C#,
The implications of the above discovery are far reaching. Firstly, for quantum field theories admitting discrete symmetries, Santilli's Theorem 3.6A implies the validity of basically new discrete symmetry that can be experimentally verified. For theories violating any discrete symmetry, Theorem 3.6A. implies that, whenever a discrete symmetry is violated, the corresponding dual symmetry has to be violated too, and vice versa.
The original 1974 paper can be downloaded from the following link
Generalization of the PCT theorem to all discrete spacetimne symmetries in quantum field theory,
R. M. Santilli and C. N. Ktorides,
Phys. Rev. D Vol. 10, 3396-3406 (1974)
The reading of the following preceding paper, also at the Phys. Rev., is instructive
Can the generalized Haag theorem be further generalized?
R. M. Santilli and C. N. Ktorides,
Phys. Rev. D Vol. 7, 2447-2456 (1973)
Ethical notes
It should be noted that the results reported above solely present the version published by Phys. Rev. and not the complete research conducted by Santilli. In essence, the editors of Phys. Rev. kept the paper for years without accepting it and without rejecting it, evidently due to the absence of a credible technical counter-arguments (in the 1970s, technical arguments were required for a rejection, something completely abandoned these days by the American and other Physical Societies that reject politically nonaligned papers without any technical motivation whatsoever).
Santilli finally understood the reason for the delay, changed the final parts, and the paper was accepted instantly. The political problems were multifold. First, there was the conclusion that, in the event a given discrete symmetry and its dual are violated, the Wightman axisoms have to be abandoned. This evident conclusion had to be remolved from the paper for its publication, as confirmed by Santilli recollections.
The biggest political proble, was, however, caused by Santilli's analytic continuation of a discrete symmetry to its connected component as expected from Lie's theory, namely, the achievement of the original goal of deriving the lack of exact character of the (continuous) Lorent transformations from the violation of a discrete symmetry. Unfortunately, the Foundation could not identify any of Santilli's original manuscripts in the field. Following consultation, Santilli released the following statment:
A direct test of the applicability or inapplicability of special relativity under conditions violating discrete symmetries was inconceivable in the 1970s as it is inconceivable today due to organized opposing interests controlling major particle laboratories around the world.
This scientific obscurantism is implemented despite the evidence that a theory, such as special relativity, that is strictly invariant under time reversal, cannot possibly be exact for a strictly irreversible process, such as a weak interactions decay, since the scattering amplitude is invariant under time reversal, thus predicting the spontaneous recombination of the debris of the decay into the original particle.
Due to this unfortunate political control of basic physical knowledge, in the 1970s I asked myself whether there was any way of establishing the lack of exact character of the connected component of the Lorentz symmetry from the violation of its discrete component. To my best recollection, I did find an analytic continuation connecting said components in such a way that the violation of one would imply that of the other.
However, for scientific honesty, I have to stress that I am not sure whether the derivation was correct due to lack of its technical review by the American Physical Society. Also, in view of the extreme complexity of the field in which I have not conducted research for some thirty years, I do not have the time to reconsider it now.
I am proud for my reputation of never accepting abuses without due response. In this particular case, the defense of the Ph. D. thesis of my student Ktorides was at stake because crucially dependent on the publication of the paper by Phys. Rev. Hence, I had to accept the political manipulation by the editors of Phys. Rev. and their referees to allow Ktorides graduation,
Following the appearance of the 1974 paper, I destroied the entire file out of sheer rage that, in a seemingly democratic country, the American Physical Society was allowed such a totalitarian control of fundamental human knowledge in complete impunity and without any control by the country .
T
The Foundation is interested in supporting research on "Santilli problem in quantum field theory," namely, whether there is an analytic continuation or other mechanism under which the violation of a discrete symmetry causes the inapplicability of the Lorentz symmetry and special relativity.
3.7. RESOLUTION OF THE HISTORICAL IMBALANCE ON ANTIMATTER (1994)
3.7A. Newton-Santilli isodual equation for antimatter
As recalled in Section 1.4, no consistent classical theory of antimatter existed prior to Santilli's research, to our best knowledge. For instance, the celebrated Newton's equation
(3.17) m dv/dt = F(t, r, v, ...)
or the celebrated Newton's gravitation
(3.18) F = g m1 m2/r2
have no means whatsoever to distinguish betweeb matter and antimatter for the very simple reason that antimatter was inconceivable at Newton's times.
Thanks to the prior discovery of his isodual mathematics outlined in Section 2, Santilli developed the isodual theory of antimatter that holds at all level of study thus restoring full democracy between matter and antimatter.
In essence, antimatter was empirical treated by merely changing the sign of the change, under the tacit assumption that antimatter exists in the same space as matter. Thus, both matter and antimatter were studied with respect to the same numbers, fields, spaces, etc. However, a correct classical representation of antimatter required a mathematics that is anti-isomorphic to that used for matter as a necessary condition to admit a charge conjugated operator image.
Santilli represents antimatter via his anti-Hermitean isodual map (2.9) that must be applied to the totality of quantities used for ,matter and all their operations. Hence, under isoduality, we have not only the change of the sign of the charge, but also the isodual conjugation of all remaining physical quantities (such as coordinates, momenta, energy, spin, etc.) and all their operations. This is the crucial feature that allows Santilli to achieve a consistent representation of antimatter also for neutral bodies.
We have in this way the Newton-Santilli isodual equation for antiparticles that we write in the simplified form
(3.19) md xd ddvd /d ddtd = Fd(td, rd, vd, ...)
where "d" denotes isodual map (2.9), and the same conjugation holds for gravitation (see below).
Note that, after working out all isodual maps, antiparticle equation(3.7) merely yields minus the value of the conventional equation for particles in both the l.h.s. and the r.h.s, thus appearing to be trivial. However, a most important feature of the above equation is that it defines antiparticles in a new space, the Euclid-Santilli isodual space, that is coexistent but different than our own space.
In this section we shall show that, starting from the fundamental equation (3.7), the isodual theory of antimatter is consistent at all subsequent levels, including quantization, at which level it is equivalent to charge conjugation.
Note that in isodual antiparticles have a negative energy. This feature is dismissed by superficial inspections as being nonphysical, thus showing venturing of judgment prior to the acquisition of technical knowledge. In fact, negative energies are indeed nonphysical, but when referred to our spacetime, that is, with respect to positive units of time, while, when referred to negative units of energy., all known objections become inapplicable, let alone resolved.
Note also that isodual antiparticles move backward in time. This view was originally suggested by Stueckelberger in the early 1900s, but dismissed because of causality problems when treated with our own positive unit of time. Santilli has shown that motion backward in time referred to a negative unit of time td is as causal as motion forward in time referred to a positive unit of time t, and this illustrates the nontriviality of the isodual map.
Moreover, the assumption that particles and antiparticles have opposing directions of time is the only one known giving hopes for the understanding of the process of annihilation of particles and their antiparticles, a mechanisms utterly incomprehensible for the 20-th century physics.
3.7B. Isodual representation of the Coulomb force
The isodual theory of antimatter verifies all classical experimental evidence on antimatter because it recovers the Coulomb law in a quite elementary way. Consider first the case of two particles with the same negative charge and Coulomb law
(3.20) F = (- q1) x (- q2) / r x r,
where the positive value of the r.h.s is assumed as representing repulsion, and the constant is assumed to have the value 1 for simplicity.
Under isoduality,y the above expression becomes
(3.21) Fd = (- q1)d xd (- q2)d /d rd xd rd,
thus reversing the sign of the equation for matter, Fd = - F. However, antimatter is referred to a negative unit of the force, charge, coordinates, etc (Section 2). Hence, a positive value of the Coulomb force referred to a positive unit representing repulsion is equivalent to a negative value of the Coulomb force referred to a negative unit, and the latter also represents repulsion.
For the case of the electrostatic force between one particle and an antiparticle, the Coulomb law must be projected either in the space of matter
(3.22) F = (- q1) x (- q2)d / r x r,
representing attraction, or in that of antimatter
(3.23) F = (- q1)d xd (- q2) /d rd xd rd,
in which case, again, we have attraction, thus representing classical experimental data on antimatter.
3.7C. Hamilton-Santilli isodual mechanics
To proceed in his reconstruction of full democracy in the treatment of matter and antimatter, Santilli had to construct the isodual image of Hamiltonian mechanics because essential for all subsequent steps. In this way he reached what is today called the Hamilton-Santilli isodual mechanics based on the isodual equations
(3.24) ddrd/dddtd = ∂dHd(rd, pd)/d∂dpd, ddpd/dddtd = - ∂dHd(rd, pd)/∂r.
and their their derivation from the isodual action Ad (a feature crucial for quantization), from which the rest of the Hamilton-Santilli isodual mechanics follows.
3.7D. Isodual special and general relativities
As indicated in Section 1.4, special and general relativities are basically unable to provide a consistent classical treatment of antimatter. Santilli has resolved this insufficiency by providing a detailed, step by step isodual liftings of both relativities with a mathematically consistent representation of antimatter in agreement with classical experimental data (see below for the quantum counterpart).
The reader should be aware that the above liftings required the prior isodual images of the Minkowskian geometry, the Poincare' symmetry and the Riemannian geometry, as well as the confirmation of the results with experimental evidence.
3.7E. Antigravity
Studies on antigravity were dismissed and disqualified in the 20-th century on grounds that ":antigravity is not admitted by Einstein's general relativity," thus resulting in a serious obscurantism because general relativity cannot represent antimatter, thus being completely disqualified for any serious statement pertaining to the gravity between matter and antimatter.
Thanks to his isodual images of special and general relativity, Santilli has restored a serious scientific process in the field, on admitting quantitative studies for all possibilities, and has shown that once antimatter is properly represented, matter and antimatter must experience antigravity (defined as gravitational repulsion) because of supporting compatible arguments at all levels of study, with no known exclusion. In fact, all known "objections" against gravitational repulsion between matter and antimatter become inapplicable under Santilli isoduality, let alone meaningless.
The arguments in favor of the above conclusion are truly forcefully because differentiated and all mutually compatible. As a trivial illustration, we have the repulsive Newton-Santilli force between a particle and an isodual particle (antiparticle) both treated in our space
(3.25) F = g x m1 x m2d / r2 = - g x m1 x m2 / r2,
which is indeed repulsive. The same conclusion is reached at all levels of study.
It should be indicated that a very compelling aspect supporting antigravity between matter and antimatter is Santilli's identification of gravity and electromagnetism indicated in Section 3.4. In fact, the electromagnetic origin of exterior gravitation mandates that gravity and electromagnetism must have similar phenomenologies, thus including both attraction and repulsion.
3.7F. Experiment on antigravity
Santilli has proposed an experiment for the final resolution as to whether antiparticles in the gravitational field of Earth experience attraction or repulsion. The experiment consists in the measure of the gravitational force of a beam of positrons in flight on a horizontal vacuum tube 10 m long at the end of which there is a scientillator. Then, the displacement due to gravity is visible to the naked eye under a sufficiently low energy (in the range of the 10-3 eV). The experiment was studied by the experimentalist Mills and shown to be feasible with current technologies and resolutory.
3.7G. Isodual quantum mechanics
Next, Santilli constructed a step-by-step image of quantum mechanics under his isodual map based on the Heisenberg-Santilli isodual time evolution for an observable Q
(3.26) id xd ddQd /d ddtd = [Q, H]d = Hd xd Qd - Qd xd Hd,
and related isodual canonical commutation rules, Schroedinger-Santilli isodual equations, etc.
He then proved that, at the operator level, isoduality is equivalent to charge conjugation.
Consequently, the isodual theory of antimatter verifies all experimental data at the operator level too. Nevertheless, there are substantial differences in treatment, such as:
1) Quantum mechanics represents antiparticles in the same space of particles, while under isoduality particles and antiparticles exist in different yet coexisting spaces;
2) Quantum mechanics represents anti[particles with positive energy referred to a positive unit, while isodual antiparticles have negative energies referred to a negative unit;
3) Quantum mechanics represents antiparticles as moving forward in time with respect to our positive time unit, while isodual antiparticles move backward in time referred to a negative unit of time.
3.7H. Experimental detection of antimatter galaxies
Recall from Section 2 that the isodual theory of antimatter was born out of Santilli's frustration as a physicist for not being able to ascertain whether a far away star, galaxy or quasar is made up of matter or of antimatter. Santilli has resolved this uneasiness via his isodual photon γd namely, photons emitted by antimatter that have a number of distinct, experimentally verifiable differences with respect to photons γ emitted by matter,
(3.27) γd ≠ γ,
thus allowing, in due time, experimental studies on the nature of far away astrophysical objects.
A most important difference between photons and their isoduals is that the latter have negative energy, as a result of which, isodual photon emitted by antimatter are predicted to be repelled in the gravitational field of matter. A possibility for the future ascertaining of the character of a far away star or quasar is, therefore, the test via neutron interferometry or other sensitive equipment, whether light from a far away galaxy is attracted or repelled by the gravitational field of Earth (for other possibilities see the literature quoted below).
3.7I. The new isoselfdual invariance of Dirac's equation
Santilli has released the following statment on the Dirac equation:
I never accepted the interpretation of the celebrated Dirac equation as presented in the 20-th century literature, namely, as representing an electron, because the (four-dimensional) Dirac's gamma matrices are generally believed to characterize the spin 1/2 of the electron. But Lie;s theory does not allow the SU(2)-spin symmetry to admit an irreducible 4-dimensional representation for spin 1/2, and equally prohibits a reducible representation close to the Dirac's gamma matrieces.
Consequently, Dirac equation cannot represent an electron intended as an elementary particle since elementarily requires the irreducible character of the representation. In the event Dirac's gamma matrices characterize a reducible representation of the SU(2)-spin, Dirac's equation must represent a composite system.
I discovered the isodual theory ofd antimatter by examining with care Dirac's equation. In this way, I noted that its gamma matrices contain a conventional two-dimensional unit I2x2 = Diag. (1, 1), as well as a conjugate negative-definoite unit - I2x2. That suggested me to construct a mathematics based on a negatiive definite unit. The isodual map come from the connection between the conventional Pauli matrices σk, k = 1, 2, 3, referred to I2x2 and those referred to - I2x2. In this way I reached the following interpretation of Dirac's gamma trices as being the tensorial product of I2x2, σk times their isoduals,
(3.28) {I2x2, σk, k = 1, 2, 3} x {I2x2d, σkd, k = 1, 2, 3}.
Therefore, I reached the conclusion that the conventional Dirac equation represents the tensoprial product of an an electron and its isodual, the positron. In particular, there was no need to use the "hole theory" or second quantization to represent antiparticles since the above re-interpretation allows full democracy between particles and antiparticles, thus including the treatment of antiparticles at the classical level, let alone in first quantization.
By continuing to study Dirac's equation withouit any preconceived notion learned from books, I discovered yet anotehr symmetry I called isoselfduality, occurring when a quantity coincides with its isodual, as it is the case for the imaginary unit id = i. In fact, Dirac's gamma matrices are isoselfdual,
(3.29) γdμ = γμ, μ = 0, 1, 2, 3.
This new invariance can have vast implications, all the way to cosmology, because the universe itself could be isoselfdual as Dirac';s equation, in the event composed of an equal amount of matter and antimatter. In conclusion, Dirac's equation is indeed one of the most important discoveries of the 20-th century with such a depth that it could eventually represent features at the particle level that actually hold for the universe as a whole.
3.7J. Isoselfdual spacetime machine
A "spacetime machine" is generally referred to a mathematical process dealing with a closed loop in the forward spacetime cone, thus requiring motions forward as well as backward in time. As such, the "machine" is not permitted by causality under conventional mathematical treatment, as well known.
Santilli discovered that isoselfdual matter, namely, matter composed by particle and their antiparticles such as the positronium, have a null intrinsic time, thus acquiring the time of their environment, namely, evolution forward in time when in a matter field, and motion backward in time when in an antimatter field.
Consequently, Santilli showed that isoselfdual systems can indeed perform a closed loop in the forward light cone without any violation of causality laws, because they can move forward when exposed to a matter and then move backward to the original starting point when exposed to an antimatter.
3.7K. Original literature
Santilli's original papers on the discocvery of isomathematics have been identified in Section 2. To our best knowledge, Santilli's first paper on the isodual theory of antimatter is the foillowing one dating to 1994 (following the 1993 paper on isodual numbers)
Representation of antiparticles via isodual numbers, spaces and geometries
R. M. Santilli,
Comm. Theor. Phys. Vol. 3, 153-181 (1994)
The first presentations of the classical isodual theory, antigrtavity, the isodual phoiton and the isoselfdual spacetimne machine appeared in the following papers
Classical isodual theory of antimatter and its
prediction of antigravity
R. M. Santilli,
Intern. J. Modern Phys. A Vol. 14, 2205-2238 (1999)
Antigravity
R. M. Santilli,
Hadronic J. Vol. 17, 257-284 (1994)
Does antimatter emit a new light?
R. M. Santilli,
Hyperfine interactions Vol. 109, 63-81 (1997)
Spacetime machine
R. M. Santilli,
Hadronic J. Vol. 17, 285-310 (1994)
An independent study by an experimentalist on the feasibility and resolutory character of the proposed measurements of the gravityu of positron in horizontal flight on Earth can be found in the following paper
Possibilities of measuring the gravitational mass of electrons and positrons in free horizontal flight
A. P. Mills,
Hadronic J. vol. 19, 77-96 (1996)
Comprehensive presentation of the isodual theory of antimatter are available in the monographs
"Elements of Hadronic Mechanics"
Vol. II: "Theoretical Foundations"
R. M. Santilli,
Ukraine Academy of Sciences (1994)
"Isodual Theory of Antimatter, with Applications to Antigravity, Grand Unification and Cosmology,"
R. M. Santilli,
Springer (2006)
Ethical notes
The serious ethically sound scholar is assumed to be aware that any theoretical or experiemntal topic that might remoteoly imply the inapplicabilityu of Eionsteiniann doctriens is strongly opposed nowdays by organzied interests in the field. Thus any expectation nowadays of the "academic acceptance" is complicity in obscurantism, at best.
Santilli ahs experienced extreme academic obstructions in merely proposing the experimental measuremnents of the gravity oif positrons in horizontal flight on Earth on the groudns indicated that "antigravity is not predicted by Einsteinian theories," even though said theories cannot represent neutral; matter or anbtiparticles, let alone represent their gravioty.
As an illustration, the test of the gravity of positrons was attempted in the 1960s at Stanford Acceleratioin cednter by W. M. Fairbanks and F. C. Witteborn via low energy positrons in vertical upward flight, but the experiment was never completed. Santilli confronted in the 1990s retired staff at SLAC who confirmned under pressure that the experiment was never completed "because of pressure by Einsteinian supporters."
Whether this is true or false, one aspect is certain: SLAC has not completed the test to this day and solely conducted to thie day to our best knwoeldge experiments fully aligned with Einsteinian doctrines. Additionally, the Nobel Laureate Burton Richther, then director of SLAC, had the audacity of prohibiting in writing a visit by Santilli to discuss his proposed test on antigravity of 1994, despite Santilli statment that he would support all costs by himself, and despite the facts that SLAC is a "national" Laboratory, Santilli being a U. S. citizen. if this is not scientific obscurantism, what else could it be?
The Foundation is interested in funding Santilli's proposal experiment to measure the gravitaty of very low energy positrons in light in a horizontal vacuum tube on Earth and is seeking experimentalists experts in the field for possible participation, but under the condition that the experiment is conducted under secrecy outside academia to prevent notorious antiscientific obstructions.
3.8. INITIATION OF q-DEFORMATIONS OF LIE THEORY
As part of his Ph. D. Thesis at the University of Torino, Italy, Santilli proposed in 1967 the first mutations (today known as "deformations") of a Lie algebra known in the mathematical and physical literature with the product
(3.30) (A, B) = p A B - q B A,
where AB is the conventional associative product, and p, q, p ± q are non-null parameters or functions. In particular, Santilli stressed in the 1967 paper that that his product (A, B) is jointly Lie-admissible (namely, (A, B) - (B, A) is Lie) and Jordan admissible (namely, (A, B) + (B, A) is Jordan),
The proposal was made as a first approximation of Lagrange and Hamilton's legacy (Section 2.1), namely, via a generalization of the analytic equations approximating external terms for open, nonconservative and irreversible systems while reconstructing ann algebra in the brackets of the time evolution.
In fact, in his 1967 paper and others of that period (see the Curriculum) Santilli writes the deformed analytic equations in the form
(3.31) dr/dt = p(∂H(r, p)/∂p), dp/dt = - q(∂H(r, p)/∂r).
that, for p = 1 and q = 1 - ε/(∂H(r, p)/∂r), Eqs. (1.2) are approximated into the form
(3.32) dr/dt = ∂H(r, p)/∂p, dp/dt = - ∂H(r, p)/∂r + ε. ε = constant,
with nonunitary time evolution of an observable Q in the finite and infinitesimal forms
(3.33) W(t) W(t)† ≠ I
(3.34) Q(t) = W(t) Q(0) Q(t)† = exp (H q t i) Q(0) exp( - i t p H),
(3.35) i dQ / dt = (Q, H) = p Q H - q H Q,
thus regaining a consistent algebra in the brackets of the time evolution, while representing, for the first time, nonconservative and irreversible systems. The lack of totally antisymmetric character of the brackets then characterize the time rate of variation of the energy
(3.36) i dH/dt = (H, H) = (p - q) HH ≠ 0,
as well as of other quantities.
In this way, Santilli realized Jordan's dream of seeing his algebras appear in physics applications, although at the level of a covering of quantum mechanics, since the latter has no possible content of Jordan algebras. Santilli also worked out the classical image of the above formulation in which the Lie-admissible character persists, although the Jordan-admissible character is lost.
Santilli's presented his mutations (deformations) of Lie algebra in the paper below via the most general possible formulation, that in which the product AB is nonassociative, with the clear identification of its associative particular form,
Embedding of Lie-algebras in nonassociative structures
R. M. Santilli, Nuovo Cimento Vol. 51, 570-576 (1967).
Subsequent vast studies in mutations were conducted as part of hadronic mechanics and, as such, they are discussed below.
Ethical notes
In 1989 L. Biebernarn and R. Macfairlane published their known paper on the simpler q-deformations with product (A, B) = AB - qBA without any quotation of Santilli's origination of 1967, even though they were fully aware of it (Biedenharn joined Santilli in the early 1980s for a DOE grant application precisely on Santilli's mutations/deformations as per documentation we hope to make available in this web site, and Macfarlane was informed directly informed by Santilli years prior to 1986).
In particular, Biedenharn and Macfairlane changed Santilli¹s original, algebraically more appropriate term of ³mutations² into ³deformations², and carefully avoided the identification of their Lie-admissible and Jordan admissible character to prevent an instantaneous identification of Santilli¹s origination, due to his known expertise in these algebras.
Following these publications, thousands of papers on q-deformations appeared in the physics literature generally without any quotation of Santilli's origination (see the legal page of this web site), as a result of which deplorable occurrence Santilli has been dubbed the most plagiarized physicists of the 20-th century.
The misconduct by Biedenharn and Macfairlane should be denounced because it offended the memory of the famed American mathematicians A. A. Albert, the originator of the notion of Lie-admissibility, not to mention the damage casued to Jordan's dream of seeing physical applications of his algebras. In fact, all q-deformations are indeed Jordan-admissible but such a property is not mentioned in the papers.
The lack of quotation of Santilli's origination by Biedenharn and Macfairlane was unfortunate for physics because the subsequent literature suppressed the Lie-admissible and Jordan admissible character of the algebra, as well as their characterization of open irreversible systems.
For an illustration, see the open denounciation Notice to Cease and Desist to the Journal of Mathematical Physics to halt manipulating references in q-deformatuions
3.9. THEOREMS OF CATASTROPHIC INCONSISTENCIES OF
NONCANONICAL AND NONUNITARY THEORIES
3.9A. The majestic consistency of Hamiltonian theories.
Santillio has always considered classical Hamiltonian mechanics and its operator image, quantum mechanics (hhereon referred to as "Hamiltonian theories") as having a majecticcconsistency, due not only to their mathematical rigour permitted by their underlying Lie's theory and its body of methods, but also to the physical consistency of their axiomatic structure.
Consider the fndamentakl dynamical equations of quantum mechanics, Heisenbverg's equations for the characterization of the time evolution of an observable Q(t) in the finitre and infinitesimal forms
(3.37) Q(t) = U(t) Q(o) Q†(t) = exp(H t i) Q(0) exp(- i t H),
(3.38) i dQ/dt = Q H - H Q = [Q, H],
(3.39) H = p2/2m + V(r) = H†, Q = Q†,
Schroedinger's equations (for h-bar = 1)
(3.40) i ∂t |> = H |> = E |>,
(3.41) pk |> = - i ∂k |>,
and the canonical commutation relations
(3.42) [ri, pj]= δij,
[ri, rj] = [pi, pj] = 0, i, j, k = 1, 2, 3.
A most dominant property for the majestic consistency is that the time evolution operator U(t) constitutes a unitary transformation when formulated on a Hilbert space over the field of complex numbers,
(3.43) U(t) U†(t) = U†(t) U(t) = I.
The corresponding property for the classical time eovclution is that of constituting a canonical transformation, that also preserves the unit.
The implications of the above simple property are far reaching. To begin, the time eovlution of quantum mechanics leaves invariant the basic unit, generally assumed to be that of the Euclidean space, I = Diag. (1, 1, 1),
(3.44) U I U&dagger ≡ I.
But the unit I = Diag. (1, 1, 1) generally represents in an abstract way units actually used in experiments, such as I = Diag. (1 cm, 1 cm, 1 cm). Consequently, the unitary character of the time evolution law of quantum mechanics implies the preservation over time of the basic units of measurements,
(3.45) I = Diag. (1 cm, 1 cm, 1 cm) → U [ Diag. (1 cm, 1 cm, 1 cm) ] U† = Diag. (1 cm, 1 cm, 1 cm).
Additionally, a quantity that is an observable (Hermitean) at the time t = 0 remains observable at all subsequent times,
(3.46) H = H† → U H U† = H' = (H')†.
Also, if quantum mechanics yields a given numerical prediction, e.g., 57.72 MeV, at a given time, the theory maintains the same numerical prediction under the same conditions at all subsequent times,
(3.47) H |> 57.72 MeV |> → U ( H |> ) U† = H' |>' = U ( 57.72 MeV |> )U† = 57.72 MeV |>'.
Finally, the unitarity of the time evolution permits the verification of causality and other physical laws. As a result, quantum mechanics has the majestic feature of preserving over time the units of measurements, the observability of physical quantities, the numerical predictions under the same conditions, causality and other nlaws. A corresponding physical consistency holds for classical Hamiltonian formulations.
3.9B. Theorems of catastrophic inconsistencies of noncanonical and nonunitary theories.
The limitations of Hamiltonian theories in face of the complexity of nature was seen in the last decades of the 20-th century by several physicists, resulting in the proposal of a considerable number of generalized theories, much along the development of hadronic mechanics.
However, unlike hadronicd mechanics, researchers generalized Hamiltonian formulations on one side, while preserving conventional mathematics. A major scientific contribution by Santilli's group has been that of identifying the inconsistencies of generalized theories conceived along these lines, that can be expressed via bthe following:
THEOREM 3.9A: All theories with a nonunitary time evolution ,
(3.48) W(t) W†(t) ≠ I,
when formulated with the mathematical methods of unitary theories (conventional fields, spaces, functional analysis, differential calculus, etc.) do not preserve said mathematical methods over time, thus being afflicted by catastrophic mathematical inconsistencies, and do not preserve over time the basic units of measurements, Hermiticity-observability, numericval predictions and causality, thus suffering of catastrophic physical inconsistencies.
Mathematical inconsistenciesL Let I be the unit of the base field at a given time t. But the time evolution cannot preserve such a unit by definition,
(3.49) I → I' = W(t) I W†(t) ≠ I.
Consequently, said theories lose the base field at subsequent times with the consequential catastrophic collapse of their entire mathematical structure.
Physical inconsistencies: Nonunitary theories do not preserve over time the basic units of measurements, because, from the very definition of a nonunitary transform, we have
(3.50) I = Diag. (1 cm, 1 cm, 1 cm) → W Diag. (1 cm, 1 cm, 1cm) W† ≠ Diag. (1 cm, 1 cm, 1 cm);
Similarly, nonunitary theories do not generally preserve observability over time, because they do not preserve Hermiticity over time in view of the Lopez lemma for which the known Hermioticity condition
(3.51) ( ψ | {H |ψ )} = { ( ψ | H } | ψ ),
is mapped under a nonunitary transform into the form
(3.52) W ( ψ | {H |ψ )} W† = ( ψ |' T { H' T | ψ )' ≠
{ ( ψ |' T H' } T | ψ ),
(3.53) T = ( W W† )-1,
due to vthe general lack of commutativity of H' and T, H' T ≠ T H'.
,p>
Also, nonunitary theories do not admit the same numerical predictions under the same conditions at different times, because, for instance, one can select a nonunitary transform for which
(3.54) Ht=0 | ψ ) = 57.72 MeV | ψ ) → W ( H | ψ ) ) W† = H' t>t | ψ )' = 9,487 MeV | ψ ),
Finally, one of Santilli's graduate students has proved that theories with a nonuunitary time evolution violate causality laws and have other catastrophic inconsistencies. Santilli then concludes by saying Nonunitary theories formulated with the mathematics of unitary theories have no mathematical or physical value of any type.
The case for classical noncanonical theories formulated with the mathematics of canonical theories have corresponding, catastrophic, mathematical and physical inconsistencieds.
3.9C Examples of catastrophically inconsistent theories.
Examples of classical catastrophically inconsistent, noncanonical theories are given by:
1) Newton's equations with nonselfadjoint (nonpotential) forces;
2) Lagrange and Hamilton analytic equations with external terms;
3) Lagrange and Hamilton;'s equations without external terms but with Lagrangian and Hamiltonian of second or hugher order (depending on accelerations or its time derivatives);
4) Birkhoffian mechanics (that, even though preserving a Lie structure, is nevertheless noncanonical);
5) Hamilton-admissible mechanics;
Examples of operator, catastrophically inconsistent nonunitary theories are:
A) (p, q)-, q-, k- or any other deformations of Lie algebras;
B) Theories with a complex-valued Hamiltonian to represent dissipativity, e.g., in nuclear physics;
C) The so-called quantum groups;
D) The so-called "squeezed states";
E) Styring theopry when including gravitation on a curved space;
F) Quantum gravity
G) Nonunitary statistics, such as that by Prigogine;
H) Supersymmetric models;
I) The Kac-Moody algebras;
and others.
The literature also contains a number of additional theories suffering of catastrophic inconsistencies not necessarily connected to nonunitarity, among which we mention the theories nonlinear in the wavefunction ψ, namely with eigenvalue equations in Hermitean Hamiltonians of the type
(3.55) H(r, p, ψ) | ψ ) = E |ψ ).
In fact, these theories violate the superpolsition principle and, consequently, cannot be consistently applierd to composite states.
Other catastrophically inconsistent theories are those with a nonassociative enveloping algebra, such as Weinberg's nonlinear theory with a time evolution of the type
(3.56) idQ/dt = Q ⊗ H - H ⊗ Q,
where Q ⊗ H is nonassociative,
because these theories cannot admnit any left and/or right unit, thus lacking the definition over a field, prohibit any meaning of measurements, lack any consistent exponentiation to reach finite transforms and hav other catastropic inconsistencies (the scholar not familiar with these occurrences should inspect in detain Section 2, see the insistence on conventional, or iso- and geno-associative enveloping algebras, and attempt their nonassociative generalizations).
Ethical notes
Numerous seemingly authoritative journals, including those of the American, British, Italian, Swedish and other societies continue to publish to this day catastrophically inconsistent theories without any indication whatsoever of the inconsistencies or their resolution in refereed journals, even following the awareness by authors and editors alieke. the pubblications simply occur in a way completely oblivious to serious science. Seer, for instance, the public denouinciation at Notice to Cease and Desist to the Journal of Mathematical Physics to halt manipulating references in q-deformatuions
Since this unreassuring trend is in violation of the most elementary rules of scienhjtific ethics, the Foundation recommend legal action against authors, editors, and poublishers in the event of lack of due correctiooins, particularly for papers published under public financial support.
3.10. SANTILLI ISO-, GENO-, AND HYPER-RELATIVITIES AND THEIR ISODUALS (1978)
3.10A. Historical notes
As indicated by W. Pauli in one of the footnotes of his famous book Theory of Relativity, H. A. Lorentz attempted in 1895 the construction via Lie's theory of the symmetry leaving invariant the locally varying speed of light within physical media, C = c/n, where c is the speed of light in vacuum and n the familiar index of refraction. However, he encountered unsurmontable difficulties, and had to restrict the study to the constancy of the speed of light in vacuum c, resulting in the now historical paper of 1904 presenting the celebrates Lorentz symmetry with connected component SO(3.1).
Santilli studied Pauli's book, identified the footnote presenting the unsolved problem, and called it the Lorentz problem, again, referring to the construction of the symmetry leaving invariant the locally varying speed of light C = c/n, such as for light traveling through liquids, atmospheres, chromospheres, etc., and initiated the research for its solution that resulted to be of such a complexity to require a lifetime of study.
By looking in retrospect, Santilli's most important contributions for Lorentz's problem have been:
1) The proof that the problem cannot be solved with Lie's theory because, even assuming that a solution is found empirically, that solution is catastrophically inconsistent in view of the Theorems of Section 3.9;
2) The construction of the iso-, geno- and hyper coverings of Lie's theory and their isoduals permitting indeed the construction of an invariant solution for physical media of matter and antimatter, respectively; and
3) Constructing step by step iso-, geno- and hyper- and isodual generalizations of all main aspects pertaining to the Lorentz symmetry, from numbers to special relativity, and proving that said covering theories verify available experimental evidence for the intended conditions of applicability.
Evidently, we cannot possibly review here this lifetime of work. Hence, we shall restrict our presentation to the sole case of isorelativity with original contributions in free pdf downloads, and merely indicate the references of the remaining relativities.
3.10B. Santilli's opening statement
For one of the seminars delivered at physics departments around the world, Santilli brought in the lecture room a small rubber ball, a glass filled up with water, a picture of far away galaxies, pictures of Sun light at the Zenith, Sunset and Sunrise, and a cigarette lighter. He then initiated the seminar with the following opening words:
Einstein's special relativity has a majestic axiomatic structure and a truly impressive body of experimental verifications for the conditions of its original conception, point-like particles and electromagnetic waves propagating in vacuum conceived as empty space. In view of these historical successes, it has been widely believed in the 20-th century that special relativity is valid for whatever conditions exist in the universe. In reality, there exist numerous conditions, beyond those of the original conception, under which special relativity is "inapplicable" and cannot be claimed to be violated for respect to Albert Einstein, because the theory was not not conceived for these broader conditions. Among a variety of these conditions, I bring to your attention the following five cases of visual evidence on the inapplicability of special relativity:
1) The squeezing of this rubber ball cannot be treated by special relativity or quantum mechanics due to their incompatibility with the deformation theory that would causes the breakdown of the central pillar of both theories, the rotational symmetry. This limitation carries on all the way to hadron physics since protons and neutrons are extended and, therefore, have to be deformable with numerous important implications, for instance, for a quantitative representation of nuclear magnetic moments;
2) The simple phenomenon of the refraction of light causing the apparent bending of the stick in this glass of water also cannot be represented with special relativity because the occurrence can be solely represented quantitatively via a decrease of the speed of light in water, thus terminating the belief on the "universal" constance of the speed of light, since its reduction to photons scattering among liquid molecules has been disqualified for lack of quantitative representation of all events for electromagnetic waves propagating in water;
3) When looking at this picture of far away galaxies, special relativity cannot provide any classical distinction between matter and and antimatter galaxies since the sole distinction admitted by special relativity is that of the sign of the charge while far away galaxies must be assumed to be neutral. At any rate, antimatter did not exist as yet at the time of Einstein's formulation of special relativity;
4) These pictures of the Sun light at the Zenith, Sunset and Sunrise constitute evidence visible to the naked eye of the inapplicability of special relativity within physical media such as our atmosphere because the first picture established the transparency of our atmosphere to blue light, thus preventing its absorption at the horizon, while the remain two pictures establish the existence of a redshift that cannot possibly follow relativity laws because, assuming it exists at Sunset, it cannot exist at Sunrise since Earth moves away from the Sun at Sunset while it moved toward the Sun at Sunrise. hence, according to special relativity, we should have a distinct redshift at Sunset and an equally distinct blueshift at Sunrise. The dominance of the redshift at both Sunset and Sunrise, therefore, establishes the existence of a basically new behavior of light propagating within physical media beyond that of light propagating in vacuum;
5) Special relativity and quantum mechanics are inapplicable to energy releasing process, such as the flame in this cigaret lighter, because all energy releasing processes are irreversible over time, while special relativity and quantum mechanics are strictly reversible and consequently predict that the flame and the smoke should recombine themselves spontaneously into the original fuel. In any case, special relativity and quantum mechanics had to be built with reversible axioms as a necessary condition to represent the physical problems in the early part of the 20-th century, such as electrons orbiting in an atomic structure. Consequently, special relativity and quantum mechanics cannot credibly be assumed as being valid for the dramatically different irreversible processes.
In this seminar I shall indicate that, thanks to the use of new mathematics specifically constructed for the problems at hand, it is possible to construct sequential coverings of special relativity and quantum mechanics providing a more adequate treatment of the above five physical conditions.
I would like to stress ab initio that I do preserve Einstein's axioms and merely present broader realizations. In different words, my way of honoring the memory of Albert Einstein is not that of adapting nature to his original formulations with consequential risk of condemnations by posterity, but instead I honor Einstein by providing a dramatic broadening of the conditions of applicability of his axioms.
In this section we provide an outline of the latter objectives as well as free pdf downloads of Santilli's original contributions at times of difficult identification in the libraries.
3.10C. Coneceptual foundations
Santilli always considered the widespread claim of the "universal constancy of the speed of light" a political posture because, as indicated in Section 1.2, the scientific statment should be "constancy of the speed of light in vacuum," since that is the sole case with experimental verifications.
He never accepted special relativit for the characterization of dynamics within physical media because most media are opaque to light. Hence, the assumption of the speed of light in vacuum as the maximal causal speed within physical media apaque to light was repugnant to him. He then searched for a geometric characterization that would replace the speed of light within physical media, in such a way to recover, of course, the speed of light when propagation returns to be in vacuum.
Santilli was also unable to accept special relativity for media that are transparent to light, such as liquids, atmospheres, chromospheres, etc., for various reasons, Consider, for instance, the propagation of light in water. In this case electrons can propagate faster than the local speed of light, producing the known Cerenkov light. He argued that, if the speed of light in vacuum is assumed as the maximal causal speed in water to salvage causality, there is the violation of a fundamental relativistic principle because the sums of two light speeds in water does not yield the speed of light in water. Alternatively, if one assumes the speed of light in water as the maximal causal speed, the relativistic addition of speeds is salvaged but special relativity would violate causality.
The usual posture of attempting to salvage special relativity via the reduction of light to photons scatteriung through atoms was dismissed as political, because such a reduction has no physical value for electromnagneticdwaves with large wavelength, such as of 1 meter wavelength, which electromagneticd waves also propagate in ater at a reducedspeed according to the law C = c/n.
By far the bioggest deviations from secial relativity are expected by Santilli within physical media that are inhomogeneous (due to a local change of density) and anisotropic (due to differences in different space directions) such as atmospheres, chromospheres, etc., because these media have geometric deviations from the honogeneity and isotropic of the Minkowski spacetime.
In studying the original contributioons, interested scholars are, therefore, suggested to pay particular attention to the interplay between geometry, algebras and physics.
3.10D. Mathematical foundations
The problem solved by Lorentz was the invariance of the Minkowskian metric m = Diag. (1, 1, 1, - c2). The problem addressed by Santilli was the invariance of the broader metric m* = Diag. (1, 1, 1, - c2/n2). it is evident that the latter metric can be solely connected to the former via a noncanonical transformations at the classical level or a nonunitary transform at the operator level. Assuming this main characteristic also assures the exiting from the class of equivalence of the Lorentz symmetry.
Hence, Santilli considered the noncanonical transform of m into the most general possible diagonal metric m* with signature (+, +, +, 1)
(3.57) m = Diag. (1, 1, 1, - c2) → m* = Diag. (1/ n12, 1/n22, 1/ n32, - c2/n42) = m* = T x m,
where the index of refraction n for the sole time component is extended to all components because generated by the mere application of the Lorentz transforms or other symmetrization processes; and the n's are called the characteristic quantities of the medium considered. The inhomogeneity of the medium is represented via a dependence of the n's on the local density μ or the local temperature τ etc., nk(r, &my;, τ, ...), k = 1, 2, 3, 4, while the anisotropy is represented by differences between the space and/ time characteristics quantities. All n's are normalized to the value nk = 1 for the vacuum.
Santilli then looked for the symmetry of the most general possible, symmetric line element in (3+1) dimension with signature (+, +, +, -)
(3.58) r*2* = ( r12/n12 + r22/n22 + r32/n32 - t2 c2/n42) E*,
where rk2 = (rk)2; assumed for isotopic element and isounit the expressions
(3.59) , ): T = Diag. (1/ n12, 1/n22, 1/n32, 1/n42) > 0,
(3.60) , ): E* = 1/T = Diag. (n12, n22, n32, n42) > 0;
formulated the theory on his iso-Minkowskian space M* (r* , x* , E*) (Section 2.6) with isocoordinates r* = r E*, r - (r1, r2, r3, t), with isoassociative product A x* B = A T B over an isofield F* with isounit E*; identified the noncanonical transform with the isounit
(3.61) W x W* = E*,
(3.62) (W x W†)-1 = T;
where † evidently represents transposed for real values matrices, and subjected to the above noncanonical transform the totality of the framework of special relativity, from numbers to physical laws, with no exclusion to avoid catastrophic inconsistencies due to mixing the mathematics of the covering theory with that of the old.
The above assumptions are sufficient to construct desired symmetry in an elementary way. In fact, the indicagted use of the noncanonical transforms permit the simple construction of: the isonumbers
(3.63) n → n* = W n W* = n (W W*) = n E*;
the isoproduct
(3.64) n m → W (n m) W* = (W n W*) (W W†)-1 (W m W†) = n* T m* = n* x* m*;
the isoexponentiation to the right and to the left for a given Lorentz generator J with related parameter w
(3.65) exp(J w xi) → W x [exp(J w i)] W† = [exp(J T w i)] E*,
(3.66) exp(- i w J) → W [exp(- i w J)] W† = E* [exp- (i w T J)] ;
consequential isotopy of the finite Lorentz transformations of a physical quantity Q(w)
(3.67) Q(w) = [exp(J w i)] Q(0) [exp(- i w J)] →
→ W { [exp(J w i)] Q(0) [exp(- i w J)] } W† =
(3.68) → [exp(J T w i)] Q*(0) [exp( - i w T J)].
All remaining needed isomathematics can be constructed in the same e;elementary way. The isodual formalism for antimatter is derived via the simple isodual transform applied to the totality of the isotopic methods (see Section 2.7 for formal treatments)
3.10E. Invariance and universality of Santilli's isotopies.
It is easy to see that the isotopic formalism of the preceding section is not invariant under both canonical and noncanonical (or unitary and nonunitary) transforms, such as
(3.69) Z Z† ≠ I,
because the above transforms does not leave invariant the basic isounit.
(3.70) E* → E'* = Z E* Z† ≠ E*,
with consequential lack of invariance of the isoproduct
(3.71) A x* B = A T B → Z (A x* B) Z† = (Z A Z†) (Z&dagger -1 T Z-1) (Z x B Z†) = A' T' B', T' ≠ T.
The above lack of basic invariances activates Theorem 3.9A with catastrophic mathematical and physical inconsistencies that should have been expected due to the mixing of isotopic methods formulated on isospaces over isofields with conventional transformations formulated on conventional spaces over conventional; fields.
it is easy to see that, if the above noncanonical or nonunitary transform is reformulated according to Santilli isomathematics, full invariance is reached and Theorem 3.9A is by[passe.
In fact, all noncanonical or nonunitary transforms can be identically reformulated in the isotopic form Z = Z* T1/2,
under which they become isocanonical or isounitary transforms, namely, they reconstruct canonicity or unitarity on isospaces over isofields,
(3.72) Z* T1/2,, Z Z† = = Z* T Z* † = Z* x* Z* † = Z* † x* Z* = E*.
It is easy to see that Santilli's isotopic formalism is indeed invariant under the above isocanonical or isounitary transform. In fact, we have the invariance of the isounit
(3.73) E * → E'* = Z* x* E* x* Z* † = Z* x* Z* † ≡ E*.
Similarly, we have the invariance of the isoproduct
(374) A* x* B* → Z* x* ( A* x* B*) x* Z* = A'* x* B'*,
namely, the isotopic element T remains unchanged. The invariance of all remaining operations then follow and Theorem 3.9A is bypassed.
The scholar serious in science should be aware that the regaining of invariance for noncanonical and nonunitary theories has been the very reason for Santilli laborious and momentum discovery and development of his isomathematics.
It is important also to know that Santilli's isotopies of the Minkowskian geometry are "directly universal" in the sense that they admit all infinitely possible mutations (deformations) of the minkowski spacetime with signature (+. +. +, -) (universality) directly in the metric without any need for coordinates transformations (direct universality).
3.10F. Lorentz-Poincare'-Santilli isosymmetry and its isodual
Following, and only following the above laborious preparatory advances, including the achievement of the crucial invariance, it was easy for Santilli to construct the isotopies of the Lorentz and Poincare'
symmetry, today known as Lorentz-Poincare'-Santilli isosymmetry. or at times Poincare'-Santilli isosymmetry. For clarity and simplicity, in this section we shall outline the projection of isospecial relativity in our spacetime. Thus, we shall continue to avoid using the the symbol "x" to denote conventional multiplication; we shall use the isomultiplication A x* B = A T B when necessary; ordinary symbols J, P, etc., will indicate quantities belonging to the Poincare' symmetry, while symbols with n asterisk will indicate quantities belonging to isospaces over isofields. To begin, the connected component of the Poincare'-Santilli isosymmetry can be written
(3.75) P*11(3.1) = [ SO*6(3.1) ⊗ T*4(a*) ] × T*1(k*),
and comprises the six-dimensional Lorentz-Santilli isosymmetry SO*6(3.1), the four-dimensional isotranslations T4(a*) in the isoparameters a = a E*and the novel one-dimensional isotopic isotransform T1(k*) in the isoparameters w* = w E* identified below, thus being eleven (rather than ten) dimensional), with conventional generators
(3.76) p*11(3.1): { Jij, Pk, Q }. i, j, k = 1, 2, 3, 4,
Lie-Santilli isocommutation rules in terms of isoproduct (2.26),
(3.77) [Jij, Jpq]* = i ( m*jp Jiq - m*ip Jjq - m*jq Jip + m*iq Jjp ),
(3.78) [Jij, Pk]* = i (mik Pj - mjk Pi ),
(3.79) [ Pij, Pij]* = [ Jij, Q]* = [P, Q]* = 0,
Casimir-Santilli isoinvariants
(3.80) C*0 = E*,
(3.81) C*2 = Pk x* P k,
(3.82) C*4 = L*k x* L* k, L*k = εijpqJjpx*Pk.
and isotransforms;
1) Isorotations (see the references for details),
(3.83) r' = R*(θ) x r;
2) Isoboosts here presented for motion in the conventional (3,4) plane
(3.84) r'1 = r1, r'2 = r2,
(3.85) r' 3 = γ* [ r3 - β* r4 (n3 / n4) ],
(3.86) r' 4 = γ* [ r4 - β* r3 ( n4 / n3) ].
(3.87) γ* = 1 / ( 1 - β* )1/2, β* = (v / n3) / (c / n4),
where v is the speed along the third axis;
3) Isotranslations,
(3.88) r'k = rk + Ak(a, ...),
(3.89) Ak = ak [ m*kk + [ m*k, Pk ] / 1! + ...] (nu sum);
4) Isotopic transform
(3.90) m* → m'* = w m*, E* → E'* = w-1 E*,
under which isoline element (3.xxx) remains indeed invariant.
In summary, recall that the Poincare' symmetry is ten dimensional. Contrary to all expectations, Santilli's isotopies of the Poincare' symmetry turned out to be eleven dimensional. Hence, Santilli conductd a re-examination of the conventional treatment of special relativity.
The basic unit of the Lorentz and Poincare' symmetries is the 4-dimensional unit matrix E = Diag. (1, 1, 1, 1) > 0, while the unit of the base field universally assumed in special relativity is the trivial unit +1. To avoid this disparity, Santilli assumed the same unit for both the symmetry and the base field, thus using a basic field with unit E. Thanks to his discovery of the isonumber theory, this assumption requires to rewrite scalars from the usual form w, into the form w* = w E (see Section 2). Consequently, one is forced to rewrite the basic invariant of special relativity in the form
(3.91) r2 = (r† m r) E =
(r12 + r22 + r32 - t2 x c2 ) E,
where r = ( rk), k = 1, 2, 3, 4, r4 = t, and rk2 = (rk)2.
These simple steps allowed the discovery that the Poincare' symmetry is eleven dimensional, rather than ten dimensional as popularly believed in the 20-th century, in view of the additional one-dimensional isotopic invariance
(3.92) ( r† m r ) E ≡ [ r† ( w m ) r ] ( w-1 E = ( r† m* r ) E*
Since all spacetime symmetries have important physical applications, the same holds for the isotopic symmetry. In fact, the new symmetry allowed Santilli to reach a basically new grand unification of electroweak and gravitational interactions, as we shall see later on.
Note that m and m* have the same signature )+. +. +. -). Hence, following the above reformulation of the conventional symmetry, we can quote the following
LEMMA 3.10A: The Poincare'-Santilli and the Poincare' symmetries are isomorphic.
The above lemma illustrates Santilli's achievement of b roader realizations of the abstract axioms of special relativity. The isodual Poincare'-Santilli isosymmetry for antimatter can be easily constructed via isoduality.
Note that the new isotopic symmetry remained undiscovered for close to one century. This should not be surprising because its discovery required the prior discovery of the isonumbers with an arbitrary unit. Note also from the direct universality of the isotopies, the Poincare'
-Santilli isosymmetry provides the invariance for all possible line elements with signature (_,. _+, +, -_, including the Riemannian, Finslerian, Non-Desarguesian and other line elements and including, as the simplest possible case, the Minkowski line element.
3.10G. Isorelativity and its isodual
Thanks to all the preceding mathematical and physical advances, Santilli has conducted a step-by-step isotopic lifting of the physical laws of special relativity resulting in a new theory today known as Santilli isorelativity. . His central assumption is, again, the preservation under isotopies of the original axioms by Einstein and only introduce a broader realization. He realized this basic condition to such an extent that special relativity and isorelativity coincide at the abstract, realization-free level so such an extent that they could be presented with the same equations only subjected to different realizations of the symbols.
The above conception is evidently permitted by Lemma 3.10A and carries far reaching physical and experimental implications because any criticism on the structure and applications of isorelativity is a criticism on Einstein's axioms, as we shall indicated later on.
Assume for simplicity that motion occurs in the (3, 4)-plane. Then, inhomogeneity of the medium is represented by a functional dependence of n3 on the local density &my;, temperature, etc., n3 = n3(r, μ, τ, ...). Anisotropy of the medium is expressed by the possible different e ns ≠ n4. Assume that motion is restricted in the (3, 4)-plane, isorelativity can be presented via the following isoaxioms presented in their projection in our spacetime with conventional multiplication:
ISOAXIOM I: The maximal causal speed within physical media is given by
(3.93) Vmax = c (n3 / n4 );
ISOAXIOMS II: The isorelativistic addition of speeds within physical media is set by the law
(3.94) Vtot = (v1 + v2) / (1 + β* 2);
ISOAXIOM III: Within physical media, time dilation, length contraction, and variation of mass with speed follow the isotopic laws
(3.95) t = γ* to,
(3.96) d = γ*-1 do,
(3.97) m = γ* mo;
AXIOM IV: Within physical media the variation of light frequency with speed follows the Doppler-Santilli isotopic law
(3.98) ω = γ* ωo;
ISOAXIOM V: Within physical media the energy equivalence of the mass follows the isotopic law
(3.99) E = m V2max.
COMMENTS: Note that the maximal causal speed is set by the geometry of the medium, namely, by the difference between the space and time characteristic functions setting up the anisotropy. As such, Vmax can be bigger, equal or smaller to the speed of light in vacuum.
The Doppler-Santilli isoshift can be either toward the blue, isoblueshift, or toward the red, isoredshift. In the former case, light acquires energy from the medium (as expected in the interior of stars), while in the latter case light releases energy to the medium (as expected in planetary atmospheres or astrophysical chromospheres). Hence, light is expected to exit a star at a frequency bigger than that of its origination, while it is expected to leave astrophysical chromospheres at a frequency smaller than that of its origination.
The celebrated equivalence principle E = m c2 is experimentally verified only for point-like particles moving in vacuum. The isoequivalence principle expresses expected differences in excess or in defect from the conventional equivalence principle depending on aid anisotropic ratio.
3.10H. Isogravitation and its isodual
As indicated in Section 2.6, one of Santilli's most important mathematical contributions has been the geometric unification of the Minkowskian and Riemannian geometries into the Minkowski-Santilli isogeometry. This unification has evidently been done as the premises for the unification of special and general relativity. In fact, Santilli's isogravitation is unique in the sense that it incorporates both special and the general relativity.
As indicated earlier, isotopic line elements include as particular cases all infinitely possible (nonsingular) Riemannian line elements. Hence, Santilli first contribution in gravitation has been the construction of a universal "symmetry of gravitation", in lieu of the 20-th century :"covariance".
The isominkowskian formulation of exterior gravitation is elementary. Any nonsingular Riemannian metric g(r) always admit the decomposition into the Minkowski metric m = Diag. (1, 1, 1, - c2) and a 4x4 dimensional positive-definite matrix Tgr(r) called gravitational isotopic element because it incorporates all gravitational features,
(3.100) g(r) = Tgr(r) m.
Santilli then assumes for basic isounit of exterior gravitation the inverse of Tgr,
(3.101) Egr* = 1 / Tgr.
The entire formal;ist of the Minkowski-Santilli isogeometry then applies, including the identical reformulation of the Einstein-Hilbert field equations, although completed with sources as in Section 3.xx.
The implications of the above discovery are far reaching and affect all quantitative sciences from classical mechanics to astrophysics. To begin, the formulation avoids the Theorems of Catastrophic Inconsistencies of Section 2.xx thanks to the invariance of isogravitation under the Poincare
-Santilli isosymmetry. The same also allows an axiomatically consistent operator formulation of gravity and grand unification, the sole known to the Foundation as being consistent.
As it is well known, all distinctions between exterior and interior gravitation were eliminated in the 20-th century for the evident intent of adapting nature to Einstein doctrines. This manipulation of science was done via the claim that interior gravitation can be reduced to a set of point-like particles under sole action at a distance, potential interactions. As an illustration of this political profile, Schwartzchild wrote two papers, one for the exterior and one for the interior gravitation, The former has been widely acclaimed in the 20-th century, while the latter has been vastly ignored because incompatible with Einstein's gravitation under a serious scrutiny.
Theorem 1.1 terminates these political postures and set the origin of macroscopic nonpotential and irreversible effects at the ultimate level of particles at short mutual distances, as a consequence of which the distinction between and inequivalence of interior and exterior problems are established beyond doubt.
For instance, the treatment of a spaceship during re-entry in atmosphere via Einstein's gravitation would be a manifest scientific corruption due to the Lagrangian character of the former and the strictly non-Lagrangian nature of the latter. In particular, the resistive forces experienced by the spaceship during re-entry is set by Theorem 1.1 to occur at the level of deep mutual penetration of the peripheral atomic electron of the spaceship and those of the surrounding atmosphere, with ensuing nonlinear, nonlocal and nonpotential interactions.
Santilli has provided the only known axiomatically correct formulation of interior isogravitation that is permitted by the complete absence of restrictions in the functional dependence of the Minkowski-Santilli isometric m*, thus allowing fir the first time in scientific history to introduce in the interior problem the local speed of light, density, temperature, and other crucial features of the interior gravitational problem whose quantitative treatment t is inconceivable in general relativity due to the excessive limitations of the Riemannian geometry.
For instance, consider any desired Riemannian metric for the exterior problem, e.g., for the exterior Schswartzchild's solution, with diagonal elements gkk, k = 1, 2, 3, 4. Then, a simple lifting of such an exterior metric to the interior problem is given by the following forms where the characteristic quantities depend on local coordinates, r, density μ, temperature τ, etc.,
(3.102) g(r, μ, τ, ...) = Diag. ( g11/n12, g22/n22, g33/n32, g44/n42) E* = Tgr(r, μ, τ, ...) m,
Following, and only following a more credible representation of interior gravitational problems, Santilli presented gravitational singularities as the zeros of the gravitational isotopic element or the infinities of the gravitational isounit,
(3.103) Gravitational Singularities: Tgr(r, μ, τ, ...) = 0, Egr(r, μ, τ, ...) → ∞.
The experimental verification of Santilli isogravity is assured by the identical reformulation of the Einstein-Hilbert field equation. However, isogravitation occurs in a flat space since the Minkowski-Santilli isospace is locally isomorphic to the minkowski space and its curvature is null. This confirms the viewpoint expressed in Section 1 according to which the Riemannian formalism provides a very elegant mathematical representation of data, but space cannot be curved in a real sense because curvature cannot explain the weight of stationary bodies, the free fall of bodies along a straight radial line, the bending of light (that is a Newtonian event), and other features.
Alternatively, Santilli has established beyond doubt that the continued insistence on space being actually curved directly causes the activation of the Theorems of Catastrophic Inconsistencies, the impossibility of reaching a consistent operator form of gravity, the impossibility o f achieving a serious grand unification of electroweak and gravitational interactions and other shortcomings of historical proportions.
3.10I. Geno- and hyper-relativities and their isoduals
As indicated in Section 1, Santilli considers irreversibility a fundamental feature of nature originating at the ultimate particle level in view of Theorem 1.1A. Isorelativity is structurally reversible and, therefore, it is considered by Santilli as a mere preparatory step toward more fundamental relativities.
It should be indicated that isorelativity has the capability of representing irreversibility via time-dependent isotopic elements T(t, r, p, E, ...) = T&dagger(t, ... ) in such a way that T(t, r, ...) ≠ T(- t, ...). However, this is a somewhat limited representational capability, In fact, isorelativity was primarily constructed to characterize closed-isolated composite systems that are stable such as the protons, thus being reversible in time, yet possess non-Hamiltonian internal effects represented with the isotopic element.
The achievement of a relativity truly capable of representing irreversibility required Santilli to construct his genomathematics with his multi-valued hyper-extension, that are structurally irreversible in the sense that they are irreversible for all possible reversible Hamiltonians. Once such a mathematics was available, new relativities followed, today known as Santilli geno- and hyper-relativities for matter and their isoduals for antimatter. We regret our inability to outline these broader relativities to prevent a prohibitive length, as well as a substantial increase in complexity of thouyght, realization and verification.
3.10L. Experimental verifications
In the arena of its applicability (dynamics within physical media or particles in conditions of deep mutual penetration), Santilli isorelativity has experimental verifications in classical physics, particle physics, nuclear physics, supuercondiuctivity, chemistry, astrophysics and cosmology (see the literature for quantitative treatments). Some of these verifications will be outlined in Sewctiuons 3.112, 3.13, 3.14.
An immediate experimental verification of isorelativity in classical physics is given by electromagnetic waves propagating in water. In this case, in this case the speed of light is given by C = c/n4, but the medium is homogeneous and isotropic, as a result of which Vmax = c, thus allowing electrons to travel faster than the local speed of light while verifying causality, and the isorelativistic sum of speeds. A similar case occurs for Newton's diffraction of light, and numerous other cases in which there is a deviation of the speed of light in vacuum.
An experimental verification in particle physics is given by the Bose-Einstein correlation outlined following the presentation of hadronic mechanics, and all other relativistic events in particle physics conventionally interpreted via the use of had hoc parameters fitted from the data. These parameters are eliminated in isorelativity and replaced with measurable quantities, such as size of particles, their density, etc. The most important verification in particle physics is the numerically exact representation of all characteristics of neutrons in their synthesis from protons and electrons as occurring in stars, which synthesis, as indicated in Section 1, admits no treatment at all via special relativity (see Section 3.12 for details).
An experimental verification in nuclear physics is given by nuclear magnetic moments that can be solely represented in an exact way via a deformation of charge distributions of protons and neutrons when members of a nuclear structure, deformations that are absolutely impossible for special relativity, but readily admitted by its covering isorelativity. Numerous other verifications also exist in nuclear physics (see Section 3.13 for details).
An experimental verification in astrophysics is given by the numerical representation of dramatically different redshifts of galaxies and quasars when physically connected according to gamma spectroscopy. For additional verifications, the serious scholar is suggested to consult the specialized literature (see Section 3.14).
3.10M. Original literature
Following decades of work, Santilli first proposed his Lie-admissible covering of Galilei and special relativities, today called genorelativities in the following 200 pages memoir of 1978 with a full identification of the isotopic particular cases, today called isorelativity,
On a possible Lie-admissible covering of Galilei's relativity in Newtonian mechanics for nonconservative and Galilei form-noninvariant systems
R. M. Santilli,
Hadronic J. Vol. 1, 223-423 (1978)
and then continued the study in more details in the following two monographs of 1978 and 1982
"Lie-Admissible Approach to the Hadronic Structure, I: Non applicability of the Galilei and Einstein Relativities,"
R. M. Santilli,
Hadronic Press (1978)
"Lie-Admissible Approach to the Hadronic Structure, II: Coverings of the Galilei and Einstein Relativities"
R. M. Santilli,
Hadronic Press (1982)
Systematic studies on isorelativity were initiated in 1983 via the following papers: 1) The first isotopies of the Lorentz symmetry on scientific record at the classical level in the paper of 1983 that includes the first known universal invariance of Riemannian line elements
Lie-isotopic lifting of special relativity
for extended deformable particles
R. M. Santilli,
Lettere Nuovo Cimento Vol. 37, 545-555 (1983)
2) The first isotopies of special relativity at the operator level also in 1983
Lie-isotopic lifting of unitary symmetries and
of Wigner's theorem for extended deformable particles,
R. M. Santilli,
Lettere Nuovo Cimento Vol. 38, 509-521 (1983)
3) The first known isotopies of the rotational symmetries presented in the following two papers of 1985 (that were written before the preceding two but were rejected by numerous jouirnals via pseudo-reviews reporetd in a page of the first paper)
Lie-isotopic liftings of Lie symmetries, I: General considerations,
R. M. Santilli,
Hadronic J. Vol. 8, 25-35 (1985)
Lie-isotopic liftings of Lie symmetries, II: Lifting of rotations,
R. M. Santilli,
Hadronic J. Vol. 8, 36-51 (1985)
4) The first isotopy of SU(2) spin appeared in the following papers of 1993 and 1998 (the second presenting intriguing application to Bell's inequality,, local realism and all that)
isotopic lifting of SU(2)-symmetry with
application to nuclear physics,
R. M. Santilli,
JINR rapid Comm. Vol. 6. 24-38 (1993)
Isorepresentation of the Lie-isotopic SU(2) algebra with application to nuclear physics and local realism,
R. M. Santilli,
Acta Appliucandae Nathematicae Vol. 50, 177-190 (1998)
5) A detailed study isotopy of the Poincare' symmetry as the universal invariance for all spacetimes with signature (+, +, +, -) was published in 1993
Nonlinear, nonlocal and noncanonical isotopies of the Poincare' symmetry,
R. M. Santilli,
Moscow Phys. Soc. Vol. 3, 255-280 (1993)
6) the first known isotopies of the spinorial covering of the Poincare' symmetry (with momentous implications in particle physics identified in the next section) appeared in the following two papers of 1993 and 1995
DUBNA PAPER to be added
Recent theoretical and experimental evidence on the apparent
synthesis of neutrons from protons and electrons, .
R. M. Santilli,
Chinese J. System Engineering and Electronics Vol. 6, 177-199 (1995)
7) The unification of special and general relativity into isorelativity was systematically studiued in the following paper ofd 1998
Isominkowskian geometry for the gravitational treatment of matter and its isodual for antimatter,
R. M. Santilli,
Intern. J. Modern Phys. D Vol. 7, 351-407 (1998)
The first systematic presentation of the isotopeis of Galilei and Einstein's relativities with the experimengtal proposal to veryufy the isoredshift appeard in the following monographs of 1991,
"Isotopic Generalization of Galilei and Einstein Relativities",
Volume I: "Mathematical Foundations"
R. M. Santilli,
Hadronic Press (1991
)
"Isotopies of Galilei and Einstein Relativities"
Vol. II: "Classical Foundations"
R. M. Santilli,
Hadronic Press (1991)
The first verification of the isodoppler shift of Santilli's isorelatiuvity predicted in the precveding two volumes was done in 1992 by R. Mignani via the numrical interpretation of dramatically different redshift of quasars when physically connected to associated galaxies
Quasar redshift in iso-Minkowski space
R. Mignani.
Physics Essays Vol. 5, 531-535 (1992)
The first studies on the direct universality of Santilli's isorelativity for all possible spacetimes with signature (+, +, +, -) are given by the following apers
Direct universality of isospecial relativity for
photons with arbitrary speeds,
R. M. Santilli,
in "Photons: Old problems in Light of New Ideas"
V. V. Dvoeglazov Editor
Nova Science (2000)
Direct universality of the Lorentz-Poincare'-Santilli
isosymmetry for extended-deformable particles,
arbitrary speeds of light and all possible spacetimes
J. V. Kadeisvili,
in "Photons: Old problems in Light of New Ideas"
V. V. Dvoeglazov Editor
Nova Science (2000
Universality of Santilli's iso-Minkowskian geometry,
A. K. Aringazin and K. M. Aringazin,
in "Frontiers of Fundamental Physics"
M. barone and F. Selleri, Editors
Plenum 91995)
The latest study on the Lie-admissible covering of special relativity for irreversible systems was presented in the memoir published by the Italian Physical Society
Lie-admissible invariant representation of irreversibility for matter and antimatter at the classical and operator level
Ruggero Maria Santilli
Nuovo Cimento B Vol. 121, p. 443-595 (2006)
Syustematic studies on both the isotopic and Lie-admissible coverings of special relativity appeared in the two memoirs of 1995 with the update below of 2008
"Elements of Hadronic Mechanics", Vol. I: "Mathematical Foundations"
R. M. Santilli
Ukraine Academy of Sciences (1993)
"Elements of Hadronic Mechanics"
Vol. II: "Theoretical Foundations"
R. M. Santilli,
Ukraine Academy of Sciences (1994)
Hadronic Mathjematics, Mechanics and Chemistry, Volume III: Iso-, Geno-, Hyper-Formulations for Matter
and Their Isoduals for Antimatter
R. M. Santilli,
Internatyional Academic Press (2008)
For various independent reviews of Santilli's iso- and geno-relativities interested scholars may consult the following monographs
"Santilli's Isotopies of Contemporary Algebras
Geometries and Relativities"
J. V. Kadeisvili,
Ukraine Academy of Sciences
Second edition (1997)
VARIOUS OTEHR MONOGRAPHS TO BE ADDED.
Ethical notes
There is no doubt that the experimental verifications of special relativity have been, not only impressive, but also emotionally overwhelming, as it is the case of the explosion of the atomic bomb on Hiroshima on August 6, 1945, confirming the validity of the equivalence principle E = m c2. No wonder that, following verifications of that magnitude, special relativity was widely assumed as being valid throughout the universe. In fact, beginning with the early part of the 20-th century, all physical research of any type in any field was adapted to verify special relativity.
However, ethically sound scholars will agree with Santilli to the effect that no matter how beautiful and valid a given theory may appear at a given time, its structural generalization is only a matter of time. With the passing of the decades, knowledge advanced progressively beyond the conditions of original conception and verification of special relativity (point-like particles and electromagnetic waves propagating in vacuum), but the validity of special relativity was imposed without a serious scrutiny.
In the second part of the 20-th century, the adaptation of nature to verify Einsteinian doctrines had reached such a dimension to create a true scientific obscurantism due to the complete lack of scrutiny on the validity of the preferred theory no matter how dramatically different the problem considered was with respect to said original conditions of conception and verification. Numerous authoritative voices of alarm began to appear, such as that by the British philosopher Karl Popper and others, including the outcry voiced by Santilli in his book of 1984
Ethical Probe of Einstein's Followers in the USA: An Insider's View
R. M. Santilli, Alpha Publishing (1984)
Documentation of the Ethical Probe
R. M. Santilli, Alpha Publishing (1985)
In essence, with the progressive increase of the complexity of the problem considered, there was the emergence of deviations from the prediction of Einsteinian theories from experimental data. These deviations were quickly "fixed" via the introduction of ad hoc parameters that were fitted from the experimental data and Einsteinian theories were then claimed to be exact.
The above process reached extremes of academic misconduct for political gains, such as the case of the Bose-Einstein correlation where, as we shall see in a subsequent section, the two point correlation functions could at best admit two arbitrary parameters, while the representation of the experimental data was achieved with fourparameters (called "chaoticity parameters") and special relativity was still claimed to be exact, while in the scientific reality the four parameters provide a direct measurement of the deviations from the basic axioms of special relativity.
During the last part of the 20-th century, the scientific obscurantism on Einsteinian doctrines had deteriorated to such a degree to be denounced as a threat to mankind due to various factors, such as: the impossibility of resolving the alarming environmental problems afflicting our planet with Einsteinian doctrines due to their reversibility compared to the irreversibility of energy releasing processes; the systematic academic suppression of any scientific democracy for qualified inquiries the world over; the impossibility of conducting any serious experimental verification of special relativity beyond the conditions of its original verifications, e.g., for irreversible particle processes; and other factors
All scientists proposing direct experimental verifications of Einsteinian doctrines, under conditions unknown during Einstein's time, were instantly disqualified, and kept away from academia, at times via illegal actions, such as the termination of tenured positions via organized academic power rather than scientific evidence.
For instance, , Santilli proposed some 18 years ago the experimental verification of the expected redshift of Sun light from the Zenith to Sunset, but the test has been and continues to be systematically ignored in astrophysical laboratories via equivocal means such as personal attacks to Santilli without any serious consideration of the test itself. The same situation occurred in all experiments proposed by Santilli over decades, such as: the verification of expected deviation from special relativity on the behavior of the meanlife of unstable particle with energy at the time of their irreversible decay; the interferometric measurement of the deformation of the charge distribution of protons and neutrons under external strong interactions expected to resolve the vexing problem of nuclear magnetic moments; the synthesis of the neutron from protons and electrons; and others.
Physics laboratories around the world have systematically and continue to prefer dramatically lesser relevant and dramatically more expensive experiments than basic tests of Einsteinian doctrines, no matter how fundamental the proposed tests are for scientific knowledge, and no matter how important for mankind are , as it is the need for new clean energies,
These occurrences identify the very essence of Santilli's scientific life and the aims of this Foundation, namely, the impossibility for a serious consideration of basic advances without a joint consideration of issues pertaining to scientific ethics and accountability.
As Santilli puts it: Following some fifty years of active research on fundamental open problems, it is my conviction that theories in physics are nowadays established by organized academic interests and definitely not by a serious scientific process. I also believe that the decay of scientific ethics and accountability has reached such a level that truly basic experiments at physics laboratories around the world can only be conducted following judicial action, due of the capillary character of organized interests on Einsteinian doctrines the world over, complete impunity guaranteed by lack of control for decades, and full support by governmental agencies funding the research.
3.9. HADRONIC MECHANICS (1967)
<3,9A. Foreword
Santilli's conception, construction, development, experimental verification, and industrial applications of hadronic mechanics, with its diversification in chemistry and biology, constitutes, without doubt, a historical scientific achievement, mostly unprecedented if one considers the novelty and variety of the needed studies by one single mind, from pure mathematics to industrial applications.
Nowadays (October 2008), hadronic mechanics constitutes a rather vast body of disciplines ranging from various covcerings of Newtonian mechanics all the way to various corresponding second quantizations, including as particular cases conventional classical and operator conservative formulations, but also admitting a sequence of branches with increasing coplexity for the treatment of matter in conditions of correspondingly increasing complexity, plus all their isoduals for antimatter.
It is evident that we can review here only the reduments of hadronic mechancs and refer the serious scholar to a seriou study of the literature made available in free pdf dowload. It should bne indicated that the primary aim of this section is the identification of Santilli's original discoveries. For all numerous subsequent contributions byh various researchers around the world. interested scholars are suggested to consult the General Bibliography on Santilli Discoveries
Historical notes
The inception of hadronic mechanics should be dated back to Santilli's Ph. D. studies in the late 1960s at the University of Torino, Italy, with the following papers
Embedding of Lie-algebras in nonassociative structures
R. M. Santilli, Nuovo Cimento Vol. 51, 570-576 (1967).
An introduction to Lie-admissible algebras
R. M. Santilli,
Supplemento al Nuovo Cimento Vol. 6, pages 1225-1249 (1968)
Dissipativity and Lie-admissible algebras
R. M. Santilli,
Meccanica, Vol. 1, pages 3-11 (1969)
and others (see Santilli's CV).
The above papers presented the first known (p, q)-deformation of quantum mechanics via the generalized dynamical equations for the representation of open irreversible systems
(3.103) Q(t) = [exp(H q t i)] Q(0) [exp(-i t p H)],
(3.104) i dQ/dt = p Q H - q H Q = (A, B),
where p, q, and p ± q are non-null scalars, possessing a joint Lie-admissible and Jordsan-admissible structure in the sense that the attached antisymmetric brackets
(3.105) [A, B] = (A, B) - (B, A)
are Lie,while the attached the symmetric brackets
(3.106) {A, B} = (A, B) - (B, A)
are Jordan.In the same paper, Santilli also proposed the classical counterpaart via the following (p, q)-deformation (called mutation) of Hamilton's equation for the representation if open c;lassical dissipative systems
(3.107) dr/dt = p ∂H/∂p, dp/dt = - q ∂H/∂r,
whose brackets of the classical time evolution are
in 1967 Santilli moved to the U. S. A. for a one year research positionb at the University of Miami, Coral Gables, Florida, funded byu N ASA. During that time he applied everywhere for a junior position in virtually all U. S. physics and mathematics departments pn gound of his studies on Lie-admissible and Jordan-admissible algebras. However, these algebras were unknown in both the mathematics and physics of the late 1960s. He then accepted a position atg the Department ofg Physics of Boston University partially funded by the U. S. Air Force (for which support he acquired the U. S. citizenship), and turned hiself to publications that in his words are typical Phys. Rev. papers nobody quotes or care for, some of which have been outlined in Sections 3.4, 3.5, 3.6, while continuing to study Lie-adsmissible and Jordan-admissible theories withoout any major publication in the field for about a decade.
In 1978 Santilli joined the the Lyman Laboratory of Physics of Harvard University following an invitation by the DOE for grant number DE-ACO2-80ER-10651.A001 (see later on the Ethical Notes for details). At that time, Santilli published the first paper proposing the construction of hadronic mechanics in his now two historical memoirs
On a possible Lie-admissible covering of Galilei's relativity
in Newtonian mechanics for nonconservative and Galilei form-noninvariant systems
R. M. Santilli, Hadronic J. Vol. 1, 223-423 (1978)
and presented its physical application in the joint memoir submitting hadronic mechanics as a covering of quantum mechanics with his lie-admissible structure
Need of subjecting to an experimental verification the validity within a hadron of Einstein special relativity and Pauli exclusion principle
R. M. Santilli, Hadronic J. Vol. 1, 574-901 (1978)
The first memoir presents a details mathematical study of Lie-admissible algebras with their Lie-isotopuic particularization, and in the second memoir presents the basic equations of hadronmic mechanic in their general Lie-admissible finmite and infinitesimal forms for open irreversible systems
(3.108) Q(t) = [exp(H S t i)] Q(0) [exp(- i t R H)],
(3.109) i dQ/dt = Q R H - H S H = (Q, H)*,
(see Eqs. , page .....ccccof xxxx) where now R, S and R ± S are nonsingular operators, that also are jointly Lie-admissible and Jordan-asdmissible.
In the same memoirs Santilli identified the Lie-isotopic particularization for closed systems with Hamiltonian and non-Hamiltonian internal forces (see below),
(3.110) Q(t) = [exp(H T t i)] Q(0) [exp(- i t T H)],
(3.111) i dQ/dt = Q T H - H T H = [Q, H]*,
(see the second 1978 memoir, eqs. xxxx. page... ), with correspondin g Birkhoffian-admissible and Birkhoffian mechanics as classical counterparts.
In thge same memoirs Santilli proposed the Birkgoffian-admissible mechanics as classical counterpart of the Lie-admissible equations and Birkhoffian mnechanics as counterpart of the Lie-0isotopic particularization, although the latetr had to be later on reformulated for various reasons identified below.
In essence, Santilli knew that time evolution (3.103) is nonunitary as a necessary condition to have a nontrivial theory. Hence, he applied a general nonuinitary transform to the same parametric deformation, and reached the general operatyor forms (3.108) and (3.109). He then applied additional noniunitary transforms and proved that the joint Lie-admissible and Jordan-admissible character perists, thus achieving in this simple way ab initioo the most general possible operator theory admitting an algebnra (as understood in mathematics) in the brackets of the time evolution (universality).
Santilli's proposal of 1978 propagated quite rapidly all over the world (despite the lack of emails at that time), and received numerous authoritative voiced of support, such as those by Nobel Laureates C. N. Yang and I. Prigogine, distinghed physicists such as S. Okubo, S. Adler, M. Froissart, and others, as well as known philosophers of science suich as K. Popper (who praised Santilli's proposal in the preface of his last book). A feverish research was t hen initiated on Santilli proposal by various mathematicians, theoreticians and experimentalists the world over (see General Bibliography on Santilli Discoveries).
Thanks to his mathematical knowledg, Santilli initiated in 1979 the representation theory of Lie-admissible algebras. Let |) be the module of a Lie-representation, e.,g., a ket belonging to a Hilbert space with right associative action Q |). In thgis case the bimodular character is trivial because the action to the left is antiisomorphic to that to the right, Q |) = - ( | Q, Q = Q†.
For the acse of Lie-admissible algebras with brackets (3.109), Santilli needed an isotopic action to the right Q S |) that is inequivalent to the to the laft (| R Q, resulting in which he called an genobymodule or Lie-admissible bimodule. These studies provoied the first known Lie-admissible fgeneralization of Schroedinger's equation
(3.) H xr |ψ )r = H R |ψ )r = E x |ψ )r,(3.xx) |ψ )r(&[psi; | |ψ )rx H = |ψ )r( ψ | S H,
that were also studied by the physicist R. Mignani in 1981 and by the mathematician H. C. Myung and Santilli in 1982 9see the indicated General Bibliography).
A large number of papers and ,onographs then followed by numerous scientists tyhe world over. However, with tyhe passing of the years Santilli was extremely dissatisfied because the Lie-admissible charactyer of the theory is indeed preserved, but the theory was not invariant under nonunitary transfropmations, thus activating the Theorems of Catastrophic inconsistencies of nonunitary theories of Section 3.9.
In particular, by the early 1990s hadronic mechanics was still incomplete due to the lack of a Lie-isotopic and Lie-admissible coverings of tghe fundamental eqiuation for the linear momentum and its action of a wavepacket (with h-bar equal to 1),
(3.xx) pi | ψ ) = - i ∂i | ψ ), ψ = exp(ki ri - E t),
(3.xx) pi | ψ ) = ki | ψ ).
As Santilli recalls, The achievement of the invariance of hadronic ,mechanics has been one of the most distressing and time consumingv research problems I ever faced because I knew that the quantum mathematics has to be entirely lifted into hadronic mathematics for any consistent trfeatment. This required the isotopical and then the genmotopiucal liuftings to reach the proper tyfreatment of the Lie-isotopic and Lie-admissible branches of hadronic mechanics, respectively.
By the early 1990s "all" main aspects pof quantum mathematics I knew had indeed been lifted, including numbers, vector and metric spaces, geometries, algebras, ggroups, representation theory, topology, etc. Nevertheless, the invariance ofd hadronic m echanics remained elusive and, most frustatingly, the lifting of the liunear momentum into forms compatible with the Lie-isotopic and Lie-admissible formu;lations escaped continuolus efforts for years by myself as well as several researchers in the field..
I remember that in early 1990s I used to control again and again all isotopic and genmotopic liftings of quantum mechanics and could not identitfy the flaw causing lack of invariance asndf had no clue on how to lift the linear momentum. This was quite distressing because hadronic mnechanics was not a complete theory without a consistent formulation pof the linear momentum eigencvalue equiations and, above all, without such a foirmulation, no experime ntal verification could be serious;lyh studied.
Finally, the teaching of the founders ofg physics came to my help. In 1994 out pof sheer distress I remembered that Newton had to buoild the differential calculus to formulate his m,echanikcs. Consequently, I finally reinspected the differential calculus still essentially unchanged since Newton';s time, to see whetehr it was indeed applicable to hadronic mechanic s and discovered that it was not because, contrary to poppular beliefs in mathematics and pohysics for centuries, conventional. differentials dr is indeed depenbdent on the base unit E of the field when the latetr has a functional dependence on the local variable, E = E(r, ...) = 1/T(r, ...) because in this case the coordinate has to be an isocoordinate r* = r E* as a result of which dr* ≠ dr. In this way I formulated the isodifferential calculus for which
(3.xx) d* r* = T* d (r E*),
∂*/&part:*r* = E* ∂/∂r*.
This discivery finally allowed me to reach a consistent formulation of the linear momentum with the isotopic expressions fully compatibvle with the corresponding Lie-isotopic and Lie-admissible liftings of Heisenberg and Schjroedinger equations
(3.xx) p*i x* | ψ* ) = p*i T | ψ* )= - i ∂*i | ψ *),, ψ* = exp(ki T ri - E T t), T = T†
(3.xx) p*i x* | ψ* ) = ki x* | ψ ).
with corresponding expression for the genotopic lifting. It was then easy to prove the desired invariance of hadronic mechanics, namely, the preservation of the basic unit, Hermiticity-ob servability, and the preservation of all numerical predictions under the same conditions at subsequentime.
After discovering that, for one entire yeat I separated msyelf from the rest of world thanks to my wife's help for fgeeding and support (without which hadronmic mechanics would never heve seen the liught), and I write the second edition of "Elements of Hadronic Mechanics, Volumes I and II that I released for publicatio n by the Ukraine Academy of Science in 1995. Following a submission in 1995, all the background mathematics was then published in 1996 by the Remdiconti Circolo Matematico Palermo. Following that time, studies on the various applications and experimental verifications of hadronic mechanics incrfeased exponentially to such a degree of maturity that, as indicated in my papers, colleagues who do not c are to participate essentially make a hiuge gift of scientific priorities to otehrs.
In summary, the main references on hadronic mechanicvs are the following: the mathematical formulations of hadronic mechanics should be see in Santilli's memoir of 1996
xxx
the first consistent formulation lof hadronic mechanicvs should be studied in the two volumes of 1995
xxx
xxx
and an update ofd 2008 cvan be found in the five volumes
xxxx
Newton-Santilli iso-, geno-, hyper equartions and their isodualsx.
Since the times of his graduate studies at the University of Torino, Italy, Santilli knew that no structural generalization of quantum mechanics was possible without a structural generalization of its physical foundations, Newton's equations. In turn, such a generalization was impossible without a basically new mathematics.
Recall that Newton's equation used in the physics of the 20-th century were restricted to those of point particles (as necessary from the local differential topology of the Euclidean space) with action at a distance forces derivable from a potential (because point particles have no collisions), since those systems are the only ones admitting quantization. Such a subclass of Newtonian system turned out to be correct, following quantization, for the description of a point-like electrons in an atomic cloud, but Santilli was interested in studying extended particles, such as a proton, in irreversible conditions when in the core of a star or, much along similar lines, in the interior of a nucleus.
The needed generalization of Newton's equations requires a representation of the actual, extended, nonspherical and deformable character of particles, plus additional contact interactions not derivable from a potential, since the latter become unavoidable as soon as point-like abstractions of particles are abandoned in favor of representation of their actual extended size. In fact, a spaceship would experience no resistance during its re-entry in atmosphere in case abstracted to a dimensionless point, while in reality the space shift experiences during re-entry a fiery resistance. Santilli expected the same conditions for the extended proton moving in the hyperdense medium inside a star.
As we shall see, by the year 1995 Santilli has achieved a sequence of structural generalizations of the mathematics of the 20-th century, but the achievement of the needed, fundamental, structural generalization of Newton's equation remained elusive. In fact, by 1995. he was able to represent the actual, extended character of the particles via a 3-dimensional realization of his isounit representing the semiaxes of a spheroid, and was indeed able to represent all well behaved, potential and nonpotential interactions, but the emerging theory remained basically incomplete.
A main reason is that the generalization of Newton's equation characterized by his isonumbers on appropriate isospaces defined below, violated the fundamental condition of invariance over time (technically, the generalized Newton's equations had to be invariant under the Lie-Santilli time isotransformation group identified below), namely, the broader equation had to yield the same numerical value under the same conditions but at different times. Instead, the broader equations continued to violated this fundamental invariance of numerical predictions over time.
Santilli has indicated that this insufficiency was the most frustrating of all his research life, because he knew that he had to subject to an isotopy the totality of the conventional mathematics, precisely to avoid inconsistencies. By 1995 he had accumulated in his file dozens of structural generalizations of Newton';s equations, none of which were published because in his words catastrophically inconsistent due to the lack of invariance over time.
Newton-Santilli isoequations
Hamilton-0Santilli isomechanics
Animalu-Santilli isoquantization
Heoisenberg-Santilli isoequations
Experimemntal verifications
Primary literature
Ethical notes
NEUTRON SYNTHESIS
MESONS SYNTHESIS
KALNAY-SANTILLI QUARK CONFINEMENT
3.10J. Absence of expansion of the universe
Clear experimental evidence establishes that light from far away galaxies is redshifted and that such a redshift increases with the distance. A widespread 20-th century interpretation of these data is that the universe is expanding at a rate that increases with the distance. A cosmological conjecture prevalent in the 20-th century was the conjecture of the "big bang" referred to a primordial explosion at the birth of the Universe. It is evident that the "big bang" conjecture can represent the cosmological redshift of galaxies, but not its increase in time, for which reasons the conjecture has seen a rapidly decreasing number of believers. Also, it is known that the "big bang" conjecture was formulated for the specific intent of preserving the validity of Einsteinian doctrines throughout the universe, in this particular case, preserve the "universal constancy of the speed of light."
Santilli's isorelativity has profound implications for our view of the Universe because it implies the lack of any expansion. In essence, interstellar space can be considered as empty to a good approximation. However, when dealing with large intergalactic distances, space is indeed a physical medium because every point of space is traversed by electromagnetic waves originating from the rest of the universe, besides space is full of particles and gases.
In this case, the Doppler-Santilli isoshift law applies, yielding a redshift, that is, a decrease of the frequency due to loss of energy to the medium. Additionally, the isoredshift evidently increases with distance due to the increased loss of energy, thus eliminating not only any expansion, but also any acceleration of the expansion with the distance. The numerical representation is then simply given by computing the value of the ratio n3/n4 from the experimental data on redshift.
Santilli's representation of the cosmological redshift of galaxies and their increase with the distance also represents the cosmological microwave background. In fact, such a radiation is nothing else that the energy released by light to intergalactic media, which energy is then continuously released as a detectable microwave radiation.
Note that Santilli does not exclude a form of expansion of the universe, provided that it is a fraction of what believed under the assumption of the "universal constancy of the speed of light". In the event the universe is constituted by half matter galaxies and half antimatter galaxies, its expansion is expected from the gravitational repulsion between matter and antimatter galaxies.
3.10K. Absence of dark matter in the universe
It is also known that the conjecture of dark matter and/or energy was yet another conjecture intended to preserve the validity of Einsteinian doctrines in the universe since the conjecture is a direct consequence of the "universal constancy of the speed of light", the validity of Einstein's equivalence principle throughout the universe, etc. without a serious inspection of their validity. Santilli isorelativity implies the elimination of dark matter and energy in the universe. To begin, Santilli first points out that, contrary to a popular belief for close to four centuries, Newton's gravitation is not universal in its historical formulation,
(3.104) F = g m1 m2 / r2,
for the evident reason that it only deals with masses, thus excluding light. However, light is indeed attracted by gravitation as stated by Newton himself in his Principia. But light only carries energy and has no mass. Hence, in order to render Newton's gravitation truly universal, Santilli has reformulated it in terms of energy, according to the law of universal gravitation
(3.105) F = s E1 E2 / r2,
(3.106) s = g / c4.
It is evident that the above reformulation eliminates any distinction between dark matter and energy, since gravitation originates from energy and not from masses.
Next, the political nature of the dark matter and energy is soon uncovered by the fact that an equal distribution of such hypothetical entity cannot possibly cause any visible or measurable effect. Consequently, to truly represent data beyond academic politics on Einsteinian doctrines, one has to assume that dark matter and energy are not uniformly distributed, but are placed here and there where pleasing pleasing Einstein's followers. Since the universal it of the entity has no measurable effect and its ad hoc distribution here and there has no credibility, Santilli never accepted the conjecture of dark matter and energy.
A numerical representation of experimental data on galaxy evolution is readily achieved if one admits the experimental reality that the space in the interior of a galaxy is indeed a physical medium much denser than the intergalactic space indicated earlier. Hence, light emitted from stars in the interior of the galaxy experiences an isoredshift that decreases progressively with the increase of the distance from the galactic center. A numerical representation of the flat character of the plot of the rotations of a galaxy as a function of the distance then provides the numerical values of the dependence of the ratio n3/n4 on the distance from the galactic center. In this way, astrophysical data on galactic dynamics are reduced to Doppler-Santilli isoredshift without any need for dark matter or energy.
Additional political adaptation of the universe to Einsteinian theories occur in the evaluation of the total energy of the universe conducted via the law E = m c2, since the latter has been only verified for point-like particles moving n vacuum or small aggregates such as nuclei. On scientific grounds, a serious astrophysical study requires the knowledge of the maximal causal speed (or its average) in the interior of stars, quasars, neutron stars, black holes and other hyperdense astrophysical objects. Said maximal causal speed is known to be much bigger than that in vacuum in the indicated hyperdense bodies. The use of Isoaxiom V terminates any need for dark energy since the "missing energy" ΔE is simply given by
(3.107) ΔE = m (V2max - c2).
For instance, by assuming as an average for the interior of all astrophysical bodies in the universe Vmax = 9.8 c, the total energy of the universe results to be 96% bigger than that computed with Einsteinian laws, without any need for dark matter or energy. Note that said value Vmax = 9.8 c is rather plausible and moderate if one considers the maximal causal speed in the interior of singularities such as black holes where Vmax is expected to be much bigger in value.
In summary, Santilli's isorelativity terminates the political adaptation of the universe to Einsteinian theories, initiate a serious scientific process in adapting the theories to astrophysical evidence, and provides a numerical representation of the universe evolution via very plausible assumptions without unacceptable ad hoc manipulation.
3.10L. Proposed astrophysical experiments
The numerical representation by isorelativity of the very large differences in cosmological redshifts of galaxies and quasars when physically connected is quite clear and simple. Quasars have extremely large chromospheres, at times bigger than our entire Solar system. Light emitted by quasars must propagate through these huge chromospheres before reaching empty space. During such a propagation, light loses energy to the medium, by therefore decreasing its speed, resulting in the Doppler-Santilli isoredshift (3.xx). The value of the ratio n3/n4 has been exactly computed for various quasars and their associated galaxies.
It should be stressed that the above calculations refer to the difference in cosmological isoredshifts. An additional isoredshift occurs for light originating from the quasar-galaxy pair but propagating through the thin intergalactic medium.
The Foundation knows of no other interpretation of the above astrophysical evidence that could compare in credibility, plausibility and scientific rigor to the above interpretation by Santilli. Scholars being aware of other similarly plausible alternatives are suggested to bring them to the attention of the Foundation for their inclusion in this web site. Note the deep interconnection between the above representation of quasars and associated galaxies and the elimination of the expansion and dark energy in the universe of the preceding section.
To verify the above results, Santilli proposed in 1991 the conduction of the following experiment: select via spectroscopic means one or more spectral lines of Sun light at the Zenith and follow them to the horizon to ascertain whether there is a measurable isoredshift due to propagation through the inhomogeneous and anisotropic atmosphere. Alternatively, it is possible to study light from a distant star before and after passing through a planetary atmosphere.
The background of the proposed experiment relates to another long standing theoretical theology without serious scientific, that is, quantitative foundation: the belief that the difference in color between Sun light at the Zenith and that at Sunset is due to scattering of photons through the atoms of the atmosphere with consequential absorptions of colors, resulting in a predominant blue at the Zenith and red at the horizon. This assumption is a theology because, in the event correct, Sun light reaching us should always be red, with light red at the Zenith and dark red at the horizon.
In any case, no scattering theory can explain the drastic change in color from the Zenith to the horizon via the sole increase of the propagation of light in atmosphere. By comparison, Santilli isorelativity provides a numerical representation of said dramatic difference in color since isoredshift is proportional to the length of propagation (as well as to density, temperature and other data).
It should be noted that Sun light at the horizon must have a conventional redshift due to the tangential speed of the rotation of Earth away from the Sun, which speed is of the order of 1,200 Km/h, thus yielding a ,measurable redshift. However, such a redshift is numerically quite small, thus unable to explain the transition of color from light blue to dark red.
The need for isoredshift emerges rather forcefully from the fact that light at Sunrise is also red despite the fact that the tangential speed due to rotation is now toward the Sun, thus causing a conventional blueshift. In reality, light at Sunrise is of a visible lesser intensity than that at the horizon. hence, such a small difference is a visual evidence of the indicated conventional Doppler's redshift. However, the dominance of read under at both Sunset and Sunrise despite opposing motion with respect to the Sun can be solely explained via Santilli's isoredshift.
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3.10M. Isotopic reconstruction of exact spacetime symmetries when conventionally broken
The physics of the 20-th century saw a rather popular interest in "symmetry breakings" for both spacetime and internal symmetries. Santilli has shown that such "breakings" are due to the use of insufficient mathematics because, when the problem at hand is treated with a more appropriate mathematics, the symmetry is reconstructed exactly and no breaking occurs.
The reconstruction of the exact SU(2)-isospin and SU(3)-color symmetries will be indicated in the next section as part of hadronic mechanics. Here we indicate Santilli's mechanism for the exact symmetry reconstruction for the case of spacetime symmetries. Consider the perfect sphere of radius 1 defined on the Euclidean space over the reals R and its known symmetry under the rotational group SO(3),
(3.108) r2 = r12 + r22 + r32 = 1 ε R.
Suppose that the above perfect sphere is elastic and experiences a deformation into an ellipsoid of the type
(3.109) r2 = r12/n12 + r22/n22 + r32/n32 ≠ 1.
It is evident that, when continued to be defined on the Euclidean space over the reals, the above deformation causes the breaking of the rotational symmetry SO(3). Santilli principle of reconstruction of the exact rotational symmetry is based on the deformation of the line element
(3.110) r2 = r12 + r22 + r32 → r12/n12 + r22/n22 + r32/n32,
while jointly submitting the basic unit of the Euclidean space E = Diag. (1, 1, 1) to the inverse deformation
(3.111) E = Diag. (1, 1, 1) → E* = Diag. (n12, n22, n32).
It is then easy to see that the definition of the deformation on the Euclid-Santilli isospace with isounit E* recovers a perfect sphere that Santilli called isosphere,
(3.112) r*2* = ( r12/n12 + r22/n22 + r32/n32) E* ε R.*.
In fact, if one semiaxis is deformed of the amount 1/nk2, but the corresponding unit is deformed of the inverse amount nk2, the numerical value of the semiaxes on isospace over isofields remains 1, with the resulting exact isosymmetry SO*(3). But the latter symmetry is isomorphic to the conventional one SO(3), thus yielding an exact reconstruction of the rotational symmetry, merely formulated with a more appropriate mathematics.
The case for the Lorentz symmetry and the discrete spacetime symmetries is handled in essentially the same manner, thus voiding the 20-th century belief that spacetime symmetries are broken, as expressed by Lemma 3.10A.
3. SANTILLI DISCOVERIES IN CHEMISTRY
3. EPILOGUE
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