A. As far as I am concerned, I never accepted Bohr's paper for scholar for various reasons, such as: 1) Bohr's objections were published in a rush only five months following the appearance of the EPR argument, thus without sufficient time for in-depth criticisms; 2) There are credible rumors that Bohr's wrote the article following pressure from German scientists who originated quantum mechanics; 3) Bohr's article is essentially motivated by the widespread political/non-scientific view that quantum mechanics can represent the entirety of the universe, expectedly, until the end of time; 4) Bohr's paper cannot be considered scientifically impeccable because he does not identify the mathematical and physical conditions under which his own view was correct; 5) The last criticism applies to all subsequent works in the field and applies in particular to the mathematical theorems by Bell, von Neumann, and others.
Q 7. What is your view on the main point of this historical controversy?
A. To my knowledge, Einstein never claimed that quantum mechanics is wrong, thus implicitly accepting its validity under given conditions. Einstein's main point was the lack of completion of quantum mechanics, namely, quantum mechanics is not the final theory of the universe due to the possible existence of a generalization "completion" (in Einstein's words) of quantum mechanics into a theory recovering classical determinism under limit conditions. I never accepted Bohr's argument or any of the large number of his followers because their denial of a possible generalization of quantum mechanics is political/non-scientific in my view.
Q 8. What is your view of Niels Bohr?
A. I believe that Bohr initiated a true scientific obscurantism which is still in full action today because the entirety of the universe, from its most minute structure to its biggest cosmological dimensions continue to be treated to this day via quantum mechanics without any consideration of its limitations, let alone the dismissal without counter-measurements of various experiments disproving its universal validity throughout the universe.
Q 9. Do you think that Niels Bohr was an antisemitic Nazi sympathizer?
A. Definitely not. Danish people are known to have opposed Nazism in any possible way and Bohr is on record to have helped various Jewish physicists to leave Germany and emigrate to the U.S.A. However, I believe that his scientific mind had been controlled by German scientists of the time because serious science is always expressed in cautious terms and every theory is known to have limitations.
Q 10. In your view, what are conditions under which criticisms of the EPR arguments are valid?
A. Bohr and all his followers tacitly assumed at the basis of their objections the most fundamental assumption of quantum mechanics namely, the approximation of particles as massive points according to Newton's original conception four centuries ago. In fact, such a silent assumption is inherent in the main equations of quantum mechanics that are notoriously based on Newton's differential calculus, namely, a calculus that can only be defined at isolated points. My inability to accept Bohr's views stems from the fact that, in the physical reality, particles are not points since they are extended, therefore deformable and hyperdense. Consequently, there are conditions (known as exterior dynamical conditions) under which particles can be approximated as massive points moving in vacuum resulting in the full validity of quantum mechanics (and Bohr's views), as it is the case for atomic structures, particles in accelerators, crystals and numerous other cases. However, there are conditions (known as interior dynamical problems) under which the approximation of particles as massive points is no longer effective, as it is the case for the structure of particles, nuclei, and stars. In fact, Enrico Fermi and numerous other distinguished scholars, expressed doubts (known to Niels Bohr) as to whether the geometry, let alone the physics of quantum mechanics is applicable to the structure of the microcosm.
Q 11. Do you have an example understandable by the general audience?
A. When two protons, as in Figure 3, are the two nuclei of the hydrogen molecule, they are in vacuum at large mutual distance, in which case said protons can indeed be effectively approximated as point particles resulting in the exact validity of quantum mechanics as well as of Bohr's view. In particular, we will never be able to achieve a measurement of their mutual distance with the precision achievable in classical mechanics. However, when the same two protons are members of a nucleus, their approximation as massive points are no longer effective as established by the fact that quantum mechanics has been unable to achieve an exact representation of nuclear data in about one century of efforts. Finally, the claim of the exact validity of quantum mechanics becomes blatantly political/non-scientific when the same two protons are in the core of a star due to the dramatic differences between the exterior conditions of the original conception and experimental verification of quantum mechanics, essentially those for massive points in vacuum, and the interior conditions here considered for two extended and hyperdense protons under extreme pressures. According to Einstein vision, it is possible that, at a limit of extreme pressures, the mutual distance between the indicated two protons in the core of a star can be identified with the same precision achievable in classical mechanics.
Q 13. Can you please outline subsequent developments?
A. It took decades for the construction, first, of the new mathematics due to the need for the completion of Newton's differential calculus from its definition at points to a definition in volumes. This was achieved in the 1996 paper Isotopies of 20th century mathematics resulting in a new mathematics known as hadronic mathematics (Amidst a large bibliography, I should mention the six volumes of Foundations of the IsoDifferential Calculus, by the mathematician S. Georgiev published by Nova Scientific Publisher). Then it took additional time for the construction of the consequential completion of quantum mechanics into a covering theory today known as hadronic mechanics and the completion of quantum chemistry into a discipline known as hadronic chemistry. Then it took a decade for the verification of the new mathematical and physical theories in various fields (see the 2016 Review of Hadronic Mechanics). Only following all that was I in a position to verify that EPR completion of quantum mechanics permitted the quantitative representation of the totality of the characteristics of the neutron in its synthesis from the hydrogen atom at the non-relativistic as well as relativistic levels (see the recent review of the neutron synthesis).
Q 14. Does your synthesis of the neutron confirm the EPR argument?.
A. The representation of the synthesis of the neutron confirms the existence of a completion of quantum mechanics we call hadronic mechanics. However, the full proof of the EPR argument requires the additional confirmation of the existence of limiting conditions under which particles recover the classical determinism. I achieved the latter proof in the 1998 paper
R. M. Santilli, "Isorepresentation of the Lie-isotopic SU(2) Algebra with Application to Nuclear Physics and Local Realism," Acta Applicandae Mathematicae Vol. 50, 177 (1998),
http://www.santilli-foundation.org/docs/Santilli-27.pdf
The first part of the proof deals with the verification that the theorems by Bell, von Neumann, and others are indeed valid under the undisclosed assumptions of dimensionless particles treated via Newton's differential calculus. The second part of the proof deals with the clarification that the indicated theorems, by no means, disprove Einstein's vision since particles are in fact extended in the physical reality. The third part of the proof deals with direct verification of the EPR argument, namely, the existence of limiting conditions under which extended particles treated via hadronic mathematics and the completion of Newton's differential calculus have identical classical counterparts.
Q 15. Did you advertise such a historical discovery?
Q 16. Can you provide an example illustrating the recovering of classical determinism?
A. Recall that we can identify the center of mass of a star or of a black hole with classical accuracy. When the two protons of Figure 3 are in their interior, their mutual distance, as well as their distance from said center of mass, is predicted to be identifiable with classical accuracy. Another example is given by the recently confirmed, negatively charged pseudoproton given by the compression of two electrons inside the neutron (Figure 7). In this case the two electrons are constrained to rotate with opposite spins within the hyperdense neutron, thus having a fixed mutual distance with classical determinism and the same holds for the distance of the electron pair from the neutron center due to very strong constraints that simply do not exist for point particles in vacuum.
Q 17. Does Einstein's vision have any new industrial applications?
A. Yes, indeed. The surpassing of quantum mechanics according to the EPR argument permits the conception, treatment and industrial development of a virtually unlimited number of new technologies. As an illustration, among several possibilities, I initiated experimental verification of the laboratory synthesis of the neutron from the hydrogen gas in early 2000. These experiments were then confirmed by numerous additional verifications, such as that of the experimental collaboration that are, de facto, experimental confirmations of Einstein's vision on the lack of final character of quantum mechanics. Recall that the neutron is one of the most important particles in nature. Hence, the capability of synthesizing a flux of neutron on demand has clear industrial relevance. Consequently thanks to the collaboration by my wife Carla Gandiglio Santilli, we did set up in early 2014 the publicly traded company Thunder Energies Corporation which is in production and sale of an equipment synthesizing neutrons on demand from a hydrogen gas called " Directional Neutron Source with a number of applications, such as the detection of nuclear material that may be concealed in baggages, the detection of precious metals in mining operations, and other uses.
Q 18. Are you studying other new technologies dependent on the EPR argument?
A. Yes. A primary reason we have been unable to achieve a controlled nuclear fusion in seventy-five years of efforts and billions of dollars of taxpayer money is that nuclei are positively charged. Consequently, nuclei experience the Coulomb repulsion which, at the distance needed for the fusion reaches astronomical values because it is proportional to the inverse square of the distance (Figure 9). At Thunder Energies Corporation we have learned how to synthesize the neutron and the negatively charged pseudoproton. We are now studying the synthesis of negatively charged nuclei that would turn the above repulsion into a very strong Coulomb attraction between nuclei, thus implying a basically new conception of controlled nuclear fusion that cannot be formulated via quantum mechanics, let alone industrially developed, while being fully treatable via the EPR completion of quantum mechanics. (see also the preceding PubRelCo Interview Jan. 2, 2019 (.
Q 19. What are your concluding remarks?
A. I believe that Einstein's vision on the lack of final character of quantum mechanics is, by far, the most important legacy by Albert Einstein because it implies a true scientific renaissance encompassing all quantitative sciences, with advances simply beyond our imagination at this writing (see the monograph New Sciences for a New Era). Therefore, I hope that colleagues will join our team in honoring Einstein's legacy of such historical proportion.
Q 20. Can you please quote other scientists who participated in the 'completion' of quantum mechanics according to the EPR argument?
A. The literature in the EPR argument is truly vast and, in my view, it should be divided into the following two classes:
Q21. The famous British philosopher of science Sir Karl Popper states in page 14 of the monograph you quote: ...... in his approach Santilli distinguishes the region of the "arena of incontrovertible applicability" of quantum mechanics (he calls it "atomic mechanics") from nuclear mechanics and hadronics, and his most fascinating argiument in support of the view that quantum mechanics should not, without new tests, be regarded as valid in nuclear and hadronic mechanics, seems to me to augur a return to sanity: to that realism and objectivism for which Einstein stood and which had been abandoned by those two very great physicists, Heisenberg and Bohr. Do you have any comment?
A. I remember that Sir Karl Popper contacted me in 1981 when I was at Harvard University and had initiated my studies on the verification of the EPR argument. The central point which he greatly supported was the need to verify experimentally the validity or invalidity of quantum mechanics within the hyperdense media inside hadrons, such as the validity of Pauli's exclusion principle under external strong interactions which I indicated beginning with the title of my 1978 Harvard paper. Such an experimental verification is the evident serious basis for the validity or invalidity or the EPR argument. It is unfortunate for America and mankind that, some thirty eight years later, the conduction of the much needed basic experiments in the interior of hadrons has been systematically opposed by academia and the available experimental evidence on the inapplicability of quantum mechanics inside hadrons continues to be dismissed and discredited with serious environmental consequences I hope to indicate in a future interview.
Q22. Could you please provide a reference on the experimental evidence of the inapplicability of quantum mechanics inside hadrons which is so crucial for the validity of the EPR argument?
================================
COMMENTS
Post 1
Dear editors, could you please contact Prof. Santilli and ask him what is the strongest evidence supporting Einstein's vision that quantum mechanics is 'incomplete'? Thanks. Cwe6io
Post 2
Dear Cwe6io, thanks for your interest and important question. I never accepted the completeness of quantum mechanics since the time of my graduate studies in physics in the 1960s at the University of Torino, Italy. In the course of time,, I have provided three proofs of increasing complexities of Einstein's vision on the lack of completeness of quantum mechanics. Here is a non-technical outline with technical references.
1) 1967 PROOF OF THE EPR ARGUMENT
FOR IRREVERSIBLE SYSTEMS OF EXTENDED PARTICLES
Inspired by Einstein, I cannot accept quantum mechanics as a final theory
because said mechanics was conceived and verified for isolated systems of point p[articles in vacuum, such as the atomic structure, thus being strictly reversible over time,. This is also established by the invariance under anti-Hermiticity (time reversal) of the brackets of the time evolution, the Lie product [A, B] = AB - BA = - [A, B]† between two Hermitean operators A, B. Consequently, quantum mechanics is completely unable to provide a consistent representation of the irreversibility over time of high energy scattering processes, nuclear fusions and all energy releasing processes in dramatic disagreement with thermodynamics. Therefore, during my graduate studies I initiated the search for a completion of quantum mechanics into a form incorporating irreversibility. After learning that the ultimate structure of quantum mechanics is given by Lie algebras I spent the entire 1965 year at various European mathematical libraries to locate a covering of Lie algebras and finally did locate Albert's notion of Lie-admissible algebras (i. e., , algebras with product (A, B) such that the attached anti-symmetric product (A, B) - (B, A) = [A, B]* is Lie). I published in 1967 my
Ph. D. Thesis
on the embedding/completion of Le algebras into their Lie-admissible covering with product (A, B) = pAB - qBA;. In subsequent works of 1967-1968, I introduced the time evolution
idA/dt = (A, H) = pABH- qHA, (1)
(where p and q are non-null scalars) which is irreversible whenever p ≠ q due to the breaking of the anti-Hermiticity of the product (A, B) ≠ -(A, B)†. When I joined Harvard University in the late 1970s under DOE support, I proposed the construction of a completion of quantum mechanics into hadronic mechanics with basic Lie-admissible algebras (A, B)* = ARB - BSA where R(t, ...) and S(-t, ...) are non-singular Hermitean operators representing the extended character of hadrons in forward and backward motion, respectively, and proposed the completion of quantum mechanics into hadronic mechanics for irreversible systems with basic dynamical equations given by the Lie-admissible generalization of Heisenberg's equations
idA/dt = (A, H)*= ARH - HSA, (2)
which are clearly irreversible for R ≠ S.
Eqs. (2) were introduced for the first time in my
1978 Harvard's paper, see Eqs. (4.15.34b), page 746, and then treated in details in the monographs with Springer-Verlag, see Volume II, 1981,
Foundations of Theoretical Mechanics, page 163. The latest presentation at Nuovo Cimento
irreversible Lie-admissible dynamics includes the proof of the universality of law (2) for all possible irreversible processes and the proof that the classical image of Eqs.. (2) is given by the Historical Lagrange's and Hamilton's equations, not the truncated form used for quantum mechanics, but the original forms with external terms representing irreversibility. Experimental verifications and industrial applications of Lie-admissible law (2) for nuclear fusions and other energy releasing processes are available in Section 3 of f the 2016
general reviews.
The point important for Cwe6io's question is that Bell's inequality, von Neumann theorem and related works cannot be consistently defined under irreversibility due to the loss of 'all' Lie algebras, let alone that of the quantum time evolution and off the SU(2) spin algebra, thus establishing the validity of Einstein's vision on the lack of completeness of quantum mechanics beyond credible doubts.
2) 1998 PROOF OF THE EPR ARGUMENT
FOR REVERSIBLE SYSTEMS OF EXTENDED PARTICLES
I never accepted the quantum mechanical description of nuclear structures as ideal spheres containing point-like nucleons because of excessive - at time embarrassing - differences between the predictions of the theory and nuclear experimental data beginning with the simplest nucleus, the deuteron. Therefore, in the same originating paper of 1978, I proposed the particular case of Lie-admissible algebras known as Lie-isotopic (or Lie-Santilli)algebras occurring for R = S = T = T† > 0 representing volumes and densities of hadrons, and Lie-isotopic brackets [A, B]* = ATB - BTA (see the latest paper on
Lie-Santilli isotheory and references quoted therein). I then proposed the simpler branch of hadronic mechanics with Lie-isotopic generalization of Heisenberg dynamical equations
idA/dt = [A, H]* = ATH - HTA , (3)
which verify the ten conventional total conservation laws. Eqs. (3) were first introduced in my
1978 Harvard's paper, see Eqs. (4.15.49), page 752, and treated in details in the two monographs, see Volume II, 1981,
Foundations of Theoretical Mechanics, page 153. The first known exact representation of nuclear magnetic moments and spins, additional experimental verifications and industrial applications of hadronic mechanics with dynamical equations (3) - when applicable - are available in Section 2 of f the 2016
general reviews. My 1998
proof of the EPR argument
came out as a natural consequence of the Lie-isotopic generalization of Lie's theory in general, and of Pauli's matrices in particular, for extended, deformable and hyperdense nucleons in conditions of partial mutual penetration with consequential under linear and non-linear, local and non-local and potential as well as non-potential interactions fully treatable by hadronic mechanics but beyound any dream of treatment via quantum mechanics .
3) 1998 PROOF OF THE EPR ARGUMENT
VIA HIDDEN VARIABLES
Another aspect of 20th century sciences I could not accept is the widespread belief that "quantum mechanics does not admit hidden variables λ," because such a belief tacitly assumes or implies our achievement of terminal mathematical knowledge. In reality, mathematics is still at its infancy and so many new mathematics remain to be discovered. In fact, the central idea of all my studies is the generalization of the conventional associative product AB into the axiom-preserving isoproduct
A*B = ATB, (4)
which implies a generalization of all mathematics I learned at the graduate school since it must be applied to all possible products, including the product of numbers, functions, matrices, operators, etc. .Then, in my view, the ensuing new mathematics provides an explicit and concrete realization of hidden variables via the simple realization
T = Diag. (λ, 1/λ), Det T = 1. (5)
My 1998 proof of the EPR argument via hidden variables then follows from realization (5), of course, under a technical knowledge of the Lie-Santilli-isotheory in general and the isotopies of Pauli's matrices in particular.
The point here important is that hidden variables are indeed prohibited by the Copenhagen realization of the basic axioms of quantum mechanics, that with the simple associative product Ab. By contrast, hidden variables are fully admitted by the basic axioms of quantum mechanics under the more general realization of the product A*B = ATB, thus explaining their true 'hidden'' character, to such an extent that quantum and hadronic mechanics coincide at the abstract, realization-free level by conception and construction.. Ruggero Maria Santilli (email: research@thunder-energies.com)
Post 3
I would like study Prof. Santilli's Lie-isotopic formulations prior to studying the more complex Lie-admissible covering. Can anybody explain to a non-expert the main assumptions used by Prof. Santilli in his 1998 proof of the EPR argument
http://www.santilli-foundation.org/docs/Santilli-27.pdf? Thank you. Csd37ty
Post 4
Csd37ty//Post 3, here are Santilli's basic assumptions you requested, mostly in his own words,:
4.1. . Hadrons must be represented as they are in nature, that is, extended, deformable and hyperdense.
4.2. Extended hadrons are in conditions of mutual penetration as occurring, for instance, in nuclei. This second condition is necessary because extended and isolated hadrons in vacuum can one well approximated as being point-like, thus verifying quantum mechanics and related uncertainties..
4..3. Under conditions 4.1. and 242, we have the non-linear, non-local and non-potential interactions playing a crucial role in Santilli's proof of the RPR argument, as you can verify. It should be recalled from Santilli's analysis that the latter non-Hamiltonian interactions cannot exist without the mutual penetration of hyperdense charge distributions.
The rest of the
http://www.santilli-foundation.org/docs/Santilli-27.pdf
can be derived from the above three basic assumptions via compatibility arguments. For instance, the conditions of non-hamiltonian character combined with the condition of time reversal invariance, restrict all possibilities to Santilli's Lie-isotopic formulations with dynamical equations (3), and the same holds for other aspects. Xwe40io
Post 5
Can anybody indicate how Prof. Santilli represented assumptions 4.1, 4.2, and 4.3 in a form as elementary as possible? Csd37ty
Post 6
Csd37ty/Post 5 if you believe that structurally new assumptions 4.1, 4.2 and 4.3 Can be represented with 20th century mathematics, I suggest you should jump in a lake to cool down. The mathematics represents said assumptions did not exist and Santilli had to build his new isomathematics to achieve the needed representation. If you want to be a "researcher," you got to sit down and study it. Xwe40io
Post 7.
Xwe40io/Post 6, I understand and agree but could you please indicate the foundations of Santilli's new isomathematics used in the proof of the EPR argument? Csd37ty
Post 8.
Hi Csd37ty/Post 7,, that's it to my knowledge. After joining the Department of Mathematics of Harvard University under DOE support, Santilli had a true stroke of genius because in one single mathematical assumption, he represented all conditions 4.1, 4.2,, and 4.3 . In fact, Santilli introduced the generalization of the product AB between "all" possible quantities A, B (numbers, functions, matrices, operators, etc.) into form (4)
(see page 160, Vol. II of Santilli's
Foundations of Theoretical Mechanics) and preceding literature)
where the quantity T , called the isotopic element, is solely restricted to be positive definite, but otherwise having an arbitrary dependence on the characteristics of the hyperdense medium considered, such as time t, coordinates r, momenta p, wavefunctions ψ, pressure τ, temperature ξ, etc.). The axiomatically important aspect s that the new product A*B (I am here copying Santilli's words) is "isotopic" in the Greek sense of remaining associative A*(B*C) = (A*B)*C.
To see the huge implications, you have to understand that extremely simple assumption (4) implies the generalization of the totality of the 20th century applied mathematics and of related physical and chemical formulations, all generalizations indicated in the above monograph being Einstein's 'completions.'.
Santilli then introduced the following realization of the isotopic element
T = Σk-=1,..,,m Diag. (1/n12, 1/n22,
1/n32,
1/n42,) e-Γ (6a)
n = n (t, r, p, ψ, τ, ξ, ...) > 0, Γ = Γ(t, r, p, ψ, τ, ξ, ...) > 0, (6b)
where n12, n22, n32 are the semiaxes of the hadron assumed as ellipsoids and n42 represents the density of the hadron considered, all n's being normalized to the value n = 1 in vacuum. As everybody can see, realization (6) represents indeed all conditions 4.1,4.2, and 4.3, the later conditions (non-Hamiltonian interactions) being represented by the exponential function. Realization (6) also represents for the first time nuclei as a collection org extended and hyperdense nucleons in conditions of partial mutual penetration (see the r.h.s. of Figure 4).
In 1993, Santilli recognized that, for consistency, isomathematics had to be formulated over new numbers, today known as santilli isonumbers n' = nU with isoproduct (4) and arbitrary unit U, called Santilli isounit,
U(t, r, p, ψ, τ, ξ, ...) = 1/T > 0 , (7)
first introduced in the paper
isonumbers. The isouni verifies indeed the axiom of a multiplicative unit, U*n' = n'*U = n'. Once isomathematics is formulated over isofields, then all scalar quantities must have the structure of an isonumber, e.g., the isocoordinates must have for consistency the form r; = rU. Among a number of independent studies and applications of Santilli isonumbers, one may consult the monograph by the Chinese mathematician
Chun-Xuan Jiang,
Foundations of Santilli Isonumber Theory,.
In 1996, santilli realized that a representation of extended, deformable and hyperdense hadrons via realization of type (5) elaborated via Newton's differential calculus is grossly inconsistent because the former is solely defined on volumes, while the latter is solely defined on points. Therefore, he had the courage of generalizing Newton's differential calculus into a form called Santilli isodifferential calculus with basic isodifferential< and isoderivative/p>
d'r' = T d (rU) = dr + rTdU, (8a)
∂' f'(r')/∂'r' = U∂ f'(r')/∂ r' (8b)
first introduced in the mathematical memoir
isodifferential calculus, that has extended, for the first time in history, Newton's differential calculus defined for isolated points into a new differential calculus defined on volumes represented by the isotopic element T or the isounit . Among a number of independent studies on Santilli isodifferential calculus, one may consult the six volumes written by the French mathematician
S. Georgiev, Foundations of the IsoDifferential Calculus,
Volumes, I, II, III, IV,V, and VI Nova Scientific Publisher (2015 on).
In his 1081 Volume II of
Foundations of Theoretical Mechanics
Santilli introduced a step by step isotopic 'completion' of
the various branches of Lie's theory, today known as the Lie-Santilli isotheory, with basic isocommutator rules
[XI , xj]* = Xi T Xj - XJ T Xi = Cijk Xk (9)
Santilli then conduscted systematic studies on the development and application of the above theory, see the 1995 monographs
Elements of Hadronic Mechanics. Among a large number of independent studies, one may consult the monograph by the 1993 Greek mathematicians
D. S. Sourlas and G. T. Tsagas
Mathematical Foundation of the
Lie-Santilli Theory.
The latter theory was then used by Santilli in 1998 for the lifting of the SU(2) spin (which is necessary to define the spin of an extended, deformable and hyperdense particle under non-Hamiltonian interactions) and consequently proved
the EPR argument.
Isomathematics is today refereed to a mathematics based on isoproduct (4), defined on an isofield with isounit (6) and elaborated with the isodifferential calculus, thus including a compatible isotopic generalization of functions, metric spaces, geometries, topologies, etc. (see the quoted paper for vast contribution by mathematicians I cannot possibly quote here).
Finally, sd37ty/Post 7 allow me to warn you against the posture assumed by some that "Santilli mathematics is too complicated." This is a non-scientific and self-disqualifying posture because the (regular branch of) isomathematics can be constructed via non-unitary transforms
W(AB)W† = A' T B',
(10a)
WW† ≠ I, A' = WAW†, B' = WBW†, T =(W W†)-1
(10b)
and the same holds for numbers, functions, Lie theory, etc. Xwe40io
Post 9
Dear Xwe40io/Post 8, could you please indicate how Prof. Santilli escaped the uncertainty principle as a necessary condition to prove the EPR argument? Thanks. Csd37ty
Post 10
Dear Csd37ty/Post 9, to answer your question you have to accept the idea of extended and hyperdense protons and neutrons in conditions of partial mutual penetration as occurring in a nuclear structure, (Figure 4 of Prof. Santilli's interview) you have to understand the emergence of nonHamiltonian forces, you have to understand the mathematics for their representation and, above all, admit that the assumption of the exact validity of Heisenberg's uncertainty in the interior of a nucleus is non-scientific The serious physics states: We do not know. After you see all the above, you have to study hadronic mechanics. Here is the gist to my knowledge. From Santilli isodifferential calculus, Eqs. (8), the hadronic isomomentum is uniquely defined by
p' * ψ'(t', r') = - i ∂' ψ'(t', r') = - i U ∂ ψ'(t', r') (11)
It is then easy to see that isolinear momenta isocommute on isospace over isofields by therefore confirming the principle of isotopies
[p'i, p'j]' =
p'i * p'j -
p'j * p'i = 0 (12)
This occurs because the isotopic element T of the isoproduct "*" , Eq. (1) cancels out with its inverse, the isounit U =1/T. However, isomomenta no longer commute in our spacetime,
[p'i, p'j] =
p'i p'j -
p'j p'i ≠ 0 (13)
because, in the absence of the isotopic product, the derivative does act non-trivially on the isounit U due to its general dependence on local coordinates, and his eliminates Heisenberg's uncertainty principle for the study of interior problems and actually replace it with a much more general principle. Cheers PS. People who thinks that this violates experimental evidence state so out of ignorance, Prof. santilli has proved that the above generalization solely holds locally in the interior of nuclei, while recovering the conventional uncertainty for their center of mass.. In fact, when isolated, nuclei represented with isotopic element (5) verify all ten total conservation laws 9see the Lorentz-Poincare'-Santilli isosymmetry in the references of Post 2).
The above expressions illustrate the crucial importance of Santilli's isodifferential calculus (8) because, in its absence, there was no possibility of achieving a consistent definition of linear momentum in hadronic mechanics. In fact, as stated various times by Prof. Santilli: Prior to the discovery of the isodifferential calculus in 1996, we had no means of confronting hadronic mechanics with experimental data because we did not know how to define its angular momentum, its basic commutation rules, etc.Xwe40io
Post 11
Dear Xwe40io/post 10 , thanks for your great help. Hoping not to abuse your time, I have one final point to understand before studying Prof. Santilli';s 1998
proof of the EPR argument.
My question is related to the general belief that quantum mechanics does not admit "hidden variables" which belief was then used as an alternative objection against the EPR argument. What is Prof. Santilli's proof that "hidden variables" do exist? Thanks again, Csd37ty
Post 12
Dear Csd37ty/Post 11, thanks for another important question deserving attention. The answer is so simple to appear trivial. Prof. Santilli proved that all basic axions of quantum mechanics admit "hidden variables" in the very notion of product. Hence, his first , and most fundamental assumption of the isoproduct Eq. (1) is an explicit and concrete realization of "hidden variables" realized via the isotopic element T in the isoproduct (4). To see it, recall that T = 1 for the conventional realization of quantum mechanics, that used by Bohr. Hence, in his 1998 paper Prof. santilli assumes Det T = 1 with concrete and explicit realization (5) of hidden variables . The third d proof of the EPR argument, that based on "hidden variables," then becomes elementary, see the 1998 paper
http://www.santilli-foundation.org/docs/Santilli-27.pdf
Good luck . Xwe40io
Post 13
I Nominated Prof. Ruggero M. Santilli for the 2019 Nobel Prize in Physics for his 1998 historical paper on the proof of the EPR argument:
R. M. Santilli, "Isorepresentation of the Lie-isotopic SU(2) Algebra with Application to Nuclear Physics and Local Realism,"
Acta Applicandae Mathematicae Vol. 50, 177 (1998), http://www.santilli-foundation.org/docs/Santilli-27.pdf. Department of Physics, University of ......., Tdf55yy
Post 14
In the e: Russian Physics Journal, Vol. 61, No. 3, July, 2018 (Russian Original No. 3, March, 2018) Quantum field approach in classical physics and geometrodynamics, V. Lasukov has shown the following:
A second-quantization treatment of the solution of the equation of classical mechanics is carried out. It is shown that all of the information about the multi-particle process of creation of a pair of scalar particles by a non-stationary potential barrier is contained in the solutions of Newton's one-particle equation. The corresponding solution does not depend on Planck's constant. It is shown that for any spatial quantum problem there exists a temporal classical analog. The obtained results can be used in quantum geometrodynamics. Qet450uo
Post 15,
My electron theory from 1983 up to 2000 deals with Einstein's GR theory completed by the principle of Thermodynamics. The surprising result and not expected at all is:
1. the mass is not a point particle
2. masse and charge both depend on the fine structure Constant
3. The FSC is derived by this theory
4. The second law reveals the nature of Quantum Gravity based on GR And explains dark matter as entropy increaser.
In one word:
The hypothesis: the electron is a point particle is wrong.
Pfdg38ty
Post 16
It seems to me that Santilli
is one of few scientists who has attempted not to to build on Quantum Mechanics, but to accept Einstein's views, and to develop his own theories. Also, as a Dane I want to point out that I agree with Santilli that Niels Bohr was absolutely not a sympathizer of the Nazis although he worked with German physicists in the early thirties. Supposedly his mother was Jewish, and the story of his sudden and dramatic escape from Nazi-occupied Denmark to England in a small plane is not unknown. He was lying on the floor of the plane barely able to stretch out. I think of science as many building blocks that never end. Vsd33iup
Post 17
My dear Bdf58hj, you want to enter into the opaque politics at Harvard University? The records at the DOE indicate that the research contracts were
administered by Harvard's MathematicsDepartment with the mathematician Prof. Shlomo Sternberg as Principal Investigator and Prof. RT. M. Santilli as co-investigator who had his office at the Department of Mathematics, Figure 5 of the PubRelCo Interview.
This is the evidence.
The additional evidence is that Prof. Santilli's mathematical discoveries
at Harvard have been superior to those of his colleagues there since the latter worked on extremely advanced yet small mathematical details, while Prof. Santilli generalized all of mathematics, as you can see from Post 8.
The rest is Harvard's opaque politics I prefer to be silent. Bdf58hj
Post 18
Einstein was right when he did not agree with the EPR experiment conclusions and had said, "spooky action at a distance"? cannot occur and that, "God does not play dice"?. See page 11:
Linear Polarization
http://vixra.org/pdf/1303.0174v5.pdf. Lwe11op
Post 19
Lwe11op/Post 18, Thank you, thank you for those refreshing memories that, unfortunately are maliciously forgotten by the establishment! cdf47uo
Post 19
I now understand from Santilli's Post 2 the reason that tsuggered the Estonia Academy of Sciences to list Santilli among the most illustrious applied mathematicians of all times with the quotation precisely of his
Ph. D. Thesis
on Lie-admissible formulations. all this occurring in 1990 under USSR domination and without any previous contact with Santilli (see Figure 10 below). The listing is self-qualifying for so many who have opposed for decades Santilli's research to honor Einstein. Bsd34o
| 
| 
Figure 10. Santilli 's 1990 Nomination by the Estonia Academy of Sciences among the most illustrious app>lied mathematicians of all times |
Post 20
It is so important that your synthesis of the neutron confirms the EPR argument. Congratulations and good luck.
I would like you to take into account that the main stream now is accepting the quantum non locality based mainly on the Alain Aspect experiment. Msd2yu
Post 21
The question raised by Msd2yu/Post 20, is important. Can anybody outline the main steps of the representation and experimental verification of the synthesis of the neutrons from the the hydrogen? Tnbaks. Bdf37si
Post 22
Hi Bdf37si/Post 21, here is what I could gather from referee3d papers. Following the construction of hadronic mechanics, and only following that, see the mionograohs
R. M. Santilli, Elements of Hadronic Mechanics,
(1995), Academy of Sciences, Kiev,
Volume I: Mathematical Foundations.
anf
Volume II: Theoretical Foundations,.,
the following refereed publications are on record:
1. The non-relativistic representation of the neutron synthesis was first achieved in the paper
. M. Santilli, "Apparent consistency of Rutherford's hypothesis on
the neutron as a compressed hydrogen atom, Hadronic J.{\bf 13}, 513
(1990).
http://www.santilli-foundation.org/docs/Santilli-21.pdf.
2. The relativistic representation of the neutron synthesis was first achieved in the paper
. M. Santilli, "Recent theoretical and experimental evidence on the
synthesis of the neutron," Communication of the JINR, Dubna, Russia, No.
E4-93-252 (1993), published in the Chinese J. System Eng. and Electr.
Vol. 6, 177 (1995)
http://www.santilli-foundation.org/docs/Santilli-18.pdf.
3. Following attempts initiated in the 1950 that failed because of lack of technical knowledge on the mechanism of the synthesis, the first experimental synthesis of the neutron in laboratory from a hydrogen gas was achieved in the paper
R. M. Santilli, "Apparent confirmation of Don Borghi's experiment on the
laboratory synthesis of neutrons from protons and electrons, Hadronic
J. {\bf 30}, 29 (2007)
http://www.i-b-r.org/NeutronSynthesis.pdf.
4. The above laboratory synthesis was confirmed by systematic tests done at
Thunder Energies Corporation..such as the test
R. M. Santilli and A. Nas, "Confirmation of the Laboratory Synthesis
of Neutrons from a Hydrogen Gas," Journal of Computational Methods in
Sciences and Eng, in press (2014)
www.thunder-energies.com/docs/neutron-synthesis-2014.pdf
5. The most recent experimental confirmation has been given by the international collaboration
Richard Norman, Anil A. Bhalekar, Simone Beghella Bartoli,
Brian Buckley, Jeremy Dunning-Davies, Jan Rak, Ruggero M. Santilli
"Experimental Confirmation of the Synthesis of Neutrons and Neutroids from
a Hydrogen Gas, American Journal of Modern Physics, Vol. 6(4-1), page 85-104 (2017)
http://www.santilli-foundation.org/docs/confirmation-neutron-synthesis-2017.pdf.
6. The above tests were generally done with five different neutron detectors identified in the quoted papers. In addition, recall that when irradiated with a neutron flux, Natural silver (Ag) is transmuted into Cadmium (Cd) and Gold (Au) is transmuted into Mercury (Hg). Santilli has provided in 2018 experimental evidence on the presence of Cd in irradiated Ag and the presence of Hg in irradiated Au, thus confirming that the
Thunder Energies Directional Neutron Source
does indeed synthesize neutrons, see the paper
R. M. Santilli,
"Apparent Experimental Confirmation of Pseudoprotons and their Application to New Clean Nuclear Energies,"
International Journal of Applied Physics and Mathematics Volume 9, Number 2, April 2019
http://www.santilli-foundation.org/docs/pseudoproton-verification-2018.pdf.
7. An independent review up to 2011 is available in the monograph
Gandzha and J. Kadeisvili, New Sciences for a New Era:
Mathematical, Physical and Chemical Discoveries of
Ruggero Maria Santilli, Sankata Printing Press,\\ Nepal (2011),
http://www.santilli-foundation.org/docs/RMS.pdf.
I hope this info is sufficient. Cheers. Ker27fi
Post 23
I agree with you that science nowadays is done via organized gangs slandering any advance over their beliefs. The slandering of Santilli's synthesis of the neutron from the hydrogen is quite easy because physicists (with due exceptions) are unaware of the complexity of the rapid DC discharge necessary to "compress" an electron inside a proton, whose achievement required three years of tests by Santilli and about half a million dollars in cost. Qualified criticism expressed in respectful language and published in refereed journals are much welcome for the advancement of our new technologies. But
crackpots moving criticisms without technical content are the enemy of science.
Dwer328hj
Post 24
I believe that Santilli address the real historical issue. Einstein, Podolski and Rosen conclude their historical paper
EPR Argument
with the statement:
While we have thus shown that the wave function does not provide a complete description of the physical reality, we left open the question of whether or not such a description exists. We believe, however, that such a theory is possible Prof. Santilli has done exact that, shown that, under a proper new dynamics for interior systems, the wave function is modified in such a way to approach classical determinism as it is the case for the two electrons of the pseudoproton, the two electron in covalence bonds, and other cases. Lfg38ty.
Post 25
Prof. Santilli, please express your view on the "EPR Paradox" as outlined, for instance, in the website
https://www.thoughtco.com/epr-paradox-in-physics-2699186. Thank you. Ysr39ui
Figure 11. A conceptual view of the entanglement of particles caused by the overlapping of their wavepackets with ensuing continuous and instantaneous communication without superluminal speeds violating special relativity |
Post 24
Dear Ysr39ui / Post 24, thank you for raising such a pertinent question. In my view, the main issue of the debate on the 'EPR paradox' is that none of the participants, including Einstein, Bohr, Bohm, Bell, and others, identified the basic assumptions of quantum mechanics underlying their claims which are essentially the following:
1) The strictly point-like characterization of particles, which is inherent in the basic calculus underlying the treatment of the paradox, Newton's differential calculus, which can be solely formulated at isolated points. The paradox of superliuminal speed in particle 'entanglements' is then a mere consequence. In my view, the EPR paradox disappears when particles and their wavepackets are admitted
to be extended and actually filling up the entire universe, of course, in a way rapidly decreasing with the distance. Hence, particles are continuously and permanently 'entangled' with their wavepackets, as illustrated in the figure, thus having continuous, thus instantaneous communications without any violation of special relativity.
2) The sole admission of interactions derivable from a potential, that is, of Lagrangian/Hamiltonian type. It appears that the 'entanglement' of wavepackets causes a 'contact interaction,' that is one without potential energy which has, nevertheless, physical implications as it is the case for a balloon moving in our atmosphere.
Following decades of search, I illustrated the interactions between entangled wavepackets in the chemical notion of valence. According to quantum mechanics and chemistry, identical electrons in singlet valence coupling must repel, rather than attract each other due to their equal charge and magnetic moments. After initial studies I initiated in the late 1970s when I was at Harvard University,
(see the chemistry debate).
I finally achieved in the late 1990s the 'attractive' force between identical valence electrons in one way and one way only, via the entanglement of their wavepackets, called 'deep mutual penetration' in the related literature (see the 2001 monograph
Foundations of Hadronic Chemistry). Besides the achievement of the first known exact representation if experimental data for the hydrogen and water molecules, the identification of an attractive force between valence electrons has permitted a deeper understanding of molecules, with the ensuing new HyperCombustion for the complete combustion of fossil fuels, which is under development by the U. S. publicly traded company
Thunder Energies Corporation
3) Insufficiency of 20th century mathematics for a consistent treatment of entangled particles. As indicated earlier, entanglements effects are strictly non-potential. Additionally, entanglement effects are strictly non-local because defined over large volumes. The treatment of entanglements via the mathematics of quantum mechanics is grossly insufficient because said mathematics is solely definable at isolated points while the entanglement volumes cannot be reduced to a finite number of isolated points. Finally, entanglement effects are non-linear, that is, depending on power and derivatives of the wavefunctions. The biggest problem of the EPR paradox is the lack of admission that 20th century mathematics simply cannot treat non-linear, non-local and non-potential effects. For this reason, I initiated at Harvard University in the 1970s the construction of a 'completion' of 20thy century applied mathematics into a form, today known as isomathematics. which has been conceived and constructed for the representation invariant over time of non-linear, non-local and non-potential effects. The main idea is truly elementary and consists in the
\generalization of all conventional product AB of arbitrary quantities A, B into the axiom-preserving, thus isotopic form ATB where T is a positive definite quantity providing the invariant representation of the extended character of wavepackets and their non-Hamiltonian interactions
(see the 1978 monographs Foundations of Theoretical Mechanics,
Volume I and
Volume II).
This initial formulation turned out to be 'incomplete' because not leaving invariant the unit '1' of the numeric field , thus requiring its formulation on numbers n* = n1* with arbitrary unit 1* = 1/T known as
isonumbers All the above efforts continued to remain 'incomplete' because, by far, the most dominant limitation of quantum mechanics is its
formulation via Newton's differential calculus, with consequential approximation of particles as isolated points. Following decades of trial and errors, I finally achieved in 1996 the 'completion' of Newton's differential calculus into a form today known as the
isodifferential calculus.
in which Newton's differential 'dr' is generalized into the broader form d*r* = Td(r 1*) = dr + rTd1*, with related derivatives, allowing the transition from the differential 'dr' at the isolated point 'r' to the isodifferential 'd*r* = Td(r1*)' which is defined over the volume T. The identification of a truly attractive force between entangled valence electrons was solely possible thanks to the use of isomathematics, and the same goes for numerous applications and experimental verifications (see the recent review
general review.
4) The general belief of the lack of existence of hidden variables. An important branch of isomathematics is the 'completion' of Lie's algebras with historical brackets [A, B] = AB - BA at the bass of the Copenhagen interpretation of quantum mechanics into the iso-Lie algebras (see the recent
review and original contributions quoted therein) with generalized brackets [A, B]* = ATB - BTA. Bohr 'hidden variables' can then be introduced very easily with the realization T = Diag. (λ, 1/λ). In the 1998 paper
proof of the EPR argument,
I presented the consequential inapplicability (and not the violation) of Bell's inequality for entangled wavepackets and the confirmation of the
EPR Argument. The point to be stressed here is that the above concrete and explicit realization of hidden variables is achieved under the full validity of quantum axioms, solely subjected to a broader realization since the abstract axioms of mathematics and isomathematics, as well as Lie theory and iso-Lie theory, are the same. What we have in reality is an interpretation of quantum mechanics broaden than the Copenhagen form, today known as hadronic mechanics (see the 1995 monographs Elements of Hadronic Mechanics,
Volume I: Mathematical Foundations.
and
Volume II: Theoretical Foundations).
5) Insufficient interest
for experimental verifications and industrial applications of the EPR argument. All studies here considered originated from the inability of quantum mechanics to achieve any quantitative representation of Rutherford's synthesis of the neutron from a proton and an electron inside a star. The representation of the neutron synthesis was solely possible via the EPR completion of quantum into hadronic mechanics. Industrial equipment synthesizing neutrons on demand from a hydrogen gas are now in production and sale by Thunder Energies Corporation.
The company is seeking nuclear physics laboratories interested in additional experimental tests and industrial applications of the ultimate process at the origin of stars, the synthesis of the neutron. Ruggero Maria Santilli, email: research(at)thunder-energies(dot)com
Post 26
May I comment that I feel the whole question of completeness relevant to several areas of theoretical physics, not just quantum mechanics although that area is certainly a definite case in point. Rather than write at length here, may I point anyone interested in the direction of the note, Completeness in Physics, by Rich Norman and myself which may be accessed quite easily on the viXra site. I think this note raises some serious questions which require answers as well as specifically mentioning the EPR Paradox.
Jeremy Dunning-Davies.
Post 27
EDITORIAL NOTE: Prof. Dunning-Davies, please provide the link for your work that we cam gladly upload. in your post Thank you.
Post 28
Dear Prof. Dunning-Davies, I agree with you fully. In fact,, as I indicated in my writings and provided examples, the confirmation of the EPR Argument and the consequential elimination of the EPR paradox (see Post 25) have direct implications in the various branches of: mathematics, physics, chemistry, biology, astrophysics, etc. Best wishes. Ruggero M. santilli
Post 29
Dear EPR Debates,
I came again across the debate and re-read some of the posts and related answers. Unfortunately I miss my posts about Goedel theorem and the ensuing discussions. These were in the page of www.galileoprincipia.org. As I see (or I think) all posts are transformed into this page except my posts and our discussion considering Goedel's theorem and the incompleteness Theorem for formal system.
I think it was a nice discussion and is at the heart of the matter.
Post 30
Dear Post 29, please send us a copy of all posts that are missing and we shall upload them immediately. Please send them at our email admin(at)eprdebates(dot)org by specifying the title of the debate you refer to. Please accept our apologies for the occurrence. It was due to our webmaster of the time leaving abruptly because of issues related to the Corona virus. We did our best to reconstruct the debate in the galileoprincipia.org which is now disconnected. The EPR Editorial Team.
Post 31
Dear Prof. Santilli
I have the following question.
How do you see the relation between your hadroinc mechanics, or the completion of quantum into hadronic mechanics and the Goedel's incompleteness theorem?
Such a question is hot debated elsewhere concerning QM, for example:
I found the following argument form Tom McFarlane, B.S. Physics, Stanford University,
see
https://www.quora.com/Is-G%C3%B6del-s-incompleteness-theorem-in-mathematics-equivalent-to-Heisenbergs-uncertainty-principle-in-physics
"Goedel's theorem is a clear-cut, either/or dichotomy: an axiomatic system of sufficient expressive power is either complete, or it is consistent. There is no partial completeness combined with partial consistency. Heisenberg's uncertainty principle, on the other hand, allows for a quantum system to have both position and momentum, provided their uncertainties are not both arbitrarily small. The more certain the position, the more uncertain the momentum, and vice versa. No such intermediate mixture exists with completeness and consistency of axiomatic systems. "
Post 32
Hello Post 31, thank you for your important question. it is true that the two Goedel's incompleteness theorems have been essentially ignored in the 20th century physics, but perhaps, having been formulated in 1931, they did not escape the attention by Albert Einstein because said theorems can be construed as precursors of the 1935 Einstein-Podolsky-Rosen argument that "quantum mechanics is not a complete theory"
http://www.eprdebates.org/docs/epr-argument.pdf.
I appreciated the request for my view, but I am afraid not to be a true expert in the indicated field because the two Goedel's incompleteness theorems do not belong to the rigorous mathematical definition definition of a "theorem" since that would require every word and/or assumption to be defined via equations. To illustrate my uneasiness as an applied mathematician, I indicate that, when applied to quantum mechanics, the second Goedel's incompleteness theorem implies that
quantum mechanics cannot demonstrate its own consistency, by therefore triggering endless epistemological discussions, outside my field of expertise as an applied mathematician, on what are the basic assumption, what is the meaning of "consistency," etc..
Regrettably, with all respect, I have the same uneasiness with the indicated view by Tom McFarlane because, when dealing with "physical" systems such as quantum mechanical particles, it is necessary to identify the basic assumptions, namely, the sole representation of said particles as being point-like while moving in vacuum under sole action-at-a-distance, potential interactions. These basic assumptions are mandated by: the potential V(r) in the Schroedinger equation which is solely defined at isolated points; the differential part of said equation which is also solely defined at isolated points; etc. Under said assumptions, Tom McFarlane view on Heisenberg's uncertainties, related Bell's inequality, etc., are indeed valid. However, point-like particles do not exist in nature. But then the admission of the actual, extended, thus deformable character of particles implies the admission of interactions (expected, e.g., in the mutual penetration of nucleons in a nuclear structure) that are non-linear (in the wavefunction), non-local (because existing in a volume that cannot be reduced to points) and definitely not derivable from a potential, thus being structurally beyond any hope of treatment via quantum mechanics, related uncertainty principle, Bell's inequality and all that.
In fact, the indicated extended representation of particles and their non-non-non interactions have allowed three different proofs of the EPR argument discussed in details at our recent international teleconference in the field, see the recording of all lectures in the website of the World Lecture Series
http://www.world-lecture-series.org/level-xii-epr-teleconference-2020. This teleconference also presented an invited talk by Evans T. D. Boney available in Section IV) delivered precisely on Goedel's incompleteness theorems and heir unreassuring implications for the standard model that may be of interest to you. In case I can be of any additional help, please do not hesitate to contact me. R. M. Santilli.
Post 33
Dear Prof Santilli, again I am glad to get your response, thank you. I do think, we understand each other well.
Now, I think with final theory here it is meant, also in the spirit of Stepfen Hawking, that we approach contentiously, with new theories and their generalization, a better and better description of the nature with models, which are capable to describe the nature, however, not or never completely. I.e . Model-dependent reality.
So, again to me completeness means the ability of reaching the final theory, which is not possible. If you, dear colleague Prof. Santilli, are able to prove a corollary to the effect that the absence of a final theory does not prohibit its completion. Fine, then my answer will be a Bohrian one, namely what do you means then with completion!.
In my view, we have to be more precise or careful, in our description and interpretation of the results of the physical theories. Clearly to avoid an overloading at least from language point of view. When the Hadronic Mechanics is a "completion" of QM to honor Einstein's memory, for me personally that is right. However, as a scientist I would say, it leads to a misunderstanding, and especially to a lot of controversies, and possibly to a confusing when such a physical theory becomes available for wide audience.
Finally, Hadronics Mechanics is a great generalization of the QM really!, to my today's understanding, because I still do not have a deep involvement in it, and so I do not see that it is a completion of QM, and I would say it is possible to introduce a hidden variable in it too (according to GOEDEL theorem, and not only), and it is then again not a completion in the same sense of EPR conclusion. Any objection is welcome!.
Post 34
Dear Post 33. Thanks for the additional comments and the nice words for hadronic mechanics, but this time we are completely disconnected because you do not appear to have inspected the refereed literature on the verification of the EPR argument and you commented before having time to view the numerous lectures in the field we just uploaded. For the record, I use he work "completion" between quotes because that is the term used by Einstein with full identification in his above quoted 1935. Unti you acquire the indicated knowledge there is no point for me to continue this contact because I cannot reproduce in a log about 50K pages of research in the field in the past century. Regards R. M. Santilli
Post 35
Dear Prof. Santilli, I am very grateful for your answer.
I have read some of your monographs and watched some of your lectures in the web,
including Evans T. D. Boney lecture form the last series in 2020. I think I understand
you very well.
In my opinion what Popper said
"A theory should be considered scientific if, and only if, it is falsifiable."
has the same contain of the Geodel incompleteness ``theorem``.
However, this concerns more or less the inability of reaching final theory.
In this respect, I do not see any contradiction to my earlier posts, which are missing!.
In the next post, I will send one of them that I found after some search my computer.
I appreciate if you post it again.
Post 36
Dear Post 36, thanks sincerely for your comments and sorry for the disappearance of various posts. The problem originated from the fact that the webmaster of the early website "galileoprincipia.org" disappeared with the passwords because of apparent family problems and we had to reconstruct the website to our best. PLEASE do send us any missing post, or their reconstruction to your best, and I will make sure they are uploaded. Regard, RMS
Post 37
I have this earlier post (updated), and hope it is valuable for the discussion of Debate 5.:
Dear Prof Santilli, I am grateful that you find the time to respond (post 36).
I am sorry not give you a reference for GOEDEL (in German "GÌÐDEL" a German
Mathematiician). See for example the following
http://www.ams.org/notices/200604/fea-davis.pdf
or https://en.wikipedia.org/wiki/G%C3%B6del%27s_incompleteness_theorems
see also in this respect (Popper words in post 35)
https://en.wikipedia.org/wiki/Karl_Popper#/media/File:Popper_gravesite.jpg
Second, I am a theoretical physicist, the conclusion about the GOEDEL
"A theory either is complete or is logical (consistency)" is very simplified.
However, in my opinion it is a mathematical theorem, fundamental and important for the discussion of the completeness of QM or any other theory.
Now, if I understand your work, the ``completed" QM is rather a generalization of the QM (and all previous physical theories).
In other word it is really not a completion or can not, because actually there exist no complete theory by considering GOEDEL theorem.
In my understanding Hadronics mechanics is a new theoretical foundation, that encompasses all previous physical theories. We will never reach a complete theory.
In Other words, or in your own words: "quantitative science will never admit final theory. No matter how beautiful any given theory may appear, its generalization is only a question of time." d encompasses all previous physical theories, including the recent one, the QM.
Post 38
Hello Post 37, thank you, for your post which I believe is important for the proof of the EPR argument. I fully agree with your view with the clarification that I am a formula man and, as such, I am not an expert in Goedel theorems. Allow me to confess that I have uneasiness with the terminology of the theorems perhaps also due to my lack of knowledge of German. In fact, when referring to an ultimate theory, I always used the word "final" and not "complete" as indicated in my quote you nicely reproduced in the post. Also, I stated various times that "Up to the early 1990s, hadronic mechanics was incomplete because of the lack of a compatible generalization of Newton-Leibnitz differential calculus." Then, in the early 2000 I stated that "The construction of hadronic mechanics was finally completed with the 1996 isotopies and genotopies of the differential calculus" but positively this does not mean that hadronic mechanics became a final theory. I remember searching the dictionary for synonyms, but could find none better than "incomplete" and "complete," while the ultimate limitations were expressed by the clear cut word "final' which does not appear to be used in the two Goedel's theorems. Incidentally. you may have noted that I restricted my research to Bell's inequality and never treated the two Goedel theorems precisely because I did not want to get involved on discussions on the meaning of the used word "complete." I am sorry but that' sall I can say in the field. Regards RMS>
Post 39
Dear Post 33 (and also Prof Santilli),We are mostly in agreement here. I agree that this generalization of Quantum Mechanics in Hadronic Mechanics is interesting primarily as a representation, alongside the Copenhagen, Many-World's and Heisenberg, each with it's own set of native insights. I would propose calling it the Heisenberg-Santilli or Heisenberg-Einstein-Santilli operator formalism of quantum mechanics, given the similarity of the T operator stuff to the Propagator in the Heisenberg formalism.
Similarly, I understand now the completion is a reference to the EPR completion, but perhaps referencing Einstein directly is a way to avoid the confusion? Because it does seem that calling things like the calculus additions necessary to maintain consistency "completions" is overwrought on its face. Because sure we've lost uncertainty and gained the vaunted completeness... but we LOST UNITARITY!?!!! And reversibility? These are nontrivial losses, and patching them up with constant renormalization is not success.
That's a problem for me. That we gain true zero uncertainty in the theory only in the limit where T is zero? Thats basically when nothing is left, or at the event horizon of a black hole. And I would add... that in those places, the old theory also has zero uncertainty! When there is nothing, we all agree it is nowhere.
Which brings me to the core concern: the focus on completion leads to an obfuscation of the core issue at hand, which is falsifiability and differentiation from the existing paradigm. If your hadronic mechanics is to cause a paradigm shift, it will need a crucial experiment, within the existing paradigm. For the isodual theory, your positrons in horizontal flight is just that. But for the hadronic mechanics, what is it? General discomfort with quark confinement? Some hand-waving about valence bonding that seems to ignore the last 40 or so years of treatments of valence bonding?
I think we can all agree that these proposed confirmations of hadronic mechanics are considerably less decisive than a positron falling up would be for isodual mechanics. Nothing I've seen shocks the conscience enough to cause a paradigm shift. And I think failure to recognize the Kuhnian nature of epistemology leads to the occasional indulgence of conspiracy talk, when really we just need to make a better case for ourselves.
Post 40
EDITORIAL NOTES: regrettably Prof. Santilli could not comment on Post 39 because the statements contained therein could not be turned into equations. Therefore, the content of the post is outside his expertise or interest. The Editors want to comment on the following statements of Post 39:
1) "....similarity of the T operator stuff to the Propagator in the Heisenberg formalism." This statement is wrong, technically and conceptually, because the isotopic operator T generalizes the structure of the basic enveloping algebra of the Copenhagen interpretation of quantum mechanics for the representation of non-Hamiltonian interactions, while Heisenberg's propagator does nothing of that. Opposing views will be posted if and only if proved with equations, namely, the proof that Heisenberg's propagators generalize the enveloping associative algebras of quantum mechanics which is a total nonsense..
2) "... but we LOST UNITARITY!?!!! And reversibility? These are nontrivial losses" This blogger implicitly claims that quantum mechanics makes no sense because unitarity makes no sense in classical mechanics ???!!! Canonical transformations are replaced by unitary transformations in the transition from classical to quantum mechanics. Exactly along the same lines, unitary transformations are replaced by the covering isounitary transformations in the transition from quantum to hadronic mechanics with full verification of causal laws, of course, in the appropriate representation spaces rather than in the spaces of other mechanics as done by this blogger for hadronic mechanics but not for quantum mechanics for some reason. The claimed "loss of reversibility" by quantum mechanics is shocking for these editors because it implies that the blogger denies the irreversibility of particle reactions. The gained Lie-admissible representation of irreversibility and related thermodynamical laws appears to be disturbing for this blogger.
3) " If your [sic] hadronic mechanics is to cause a paradigm shift, it will need a crucial experiment, within the existing paradigm." The editors believe that this blogger mimics for some reason a lack of knowledge of the numerous experimental verifications of hadronic mechanics squarely "within the existing paradigm" because none of them can be formulated with quantum mechanics (see http://www.santilli-foundation.org/docs/elements-hadronic-mechanics-iii.compressed.pdf). The Editors.
Post 41
correction to post 37: I am sorry it is and also was (post 32), not (post 36)
Post 42
The guy of post 39 is out of whack. The isotopic (= axiom-preserving) branch of hadronic mechanics verifies unitarity and reversibility in the appropriate space,
Post 43
It seem so me that post 39 confirms Prof. Santilli's quote The most ascientific process of contemporary societies is the scientific process "http://www.eprdebates.org/santilli-quotes.php,
Post 44
Post 39 dubs "band-waving" the first attraction between valence pairs in molecular bonds (Post 39 now has repulsion....!!!!) and its first exact representation of experimental data for H2 and H2O (Post 39 has only approximate values....!!!) and he calls all this "hand-waving" ??? !!!, No wonder Post 40 justly speaks of mimicking !!!.
Post 45
Post 39. I agree with the most of your comment. The fact that we gain true zero uncertainty in the theory only in the limit where T is zero, is an important point.
I have the following example and hope it applies for this case (T->0) or I am not mistaken in my statement. By considering information extracted by the experimenter (observer)form a system (atom) by detecting light, the condition T->0 can only be satisfied when the observation apparatus and the atom become close that mutual penetration is large enough. However, at this condition the atom and the apparatus become one-system and the observer can not get any information form the apparatus. That is why I am skeptic to accept Santilli proof of the lose of UNCERTAINTY!.
Post 46
Post 45, Einstein was skeptic as to whether quantum uncertainties are complete=final, so you are not alone to have skepticisms, but then you need credible technical arguments. The separation between politics and serious science is set by the question: do you have a formulation better than Santilli's hadronic mechanics for the uncertainties of particles in deep entanglement? Of course not. Hence you beg for a claim on the political intent of your view. This seems to be confirmed by your statement "Santilli proof of the lose [loss] of UNCERTAINTY!." I do not claim to be an expert theoretician, but it seems very clear that hadronic mechanics is a covering of quantum mechanics which is recovered uniquely and unambiguously for mutual distances "r" of particles bigger than the hadronic horizon. In plain language, hadronic mechanics recovers conventional uncertainties in full for sufficiently large values of "r" for which T = 1 under which all the old stuff you like comes back. So where is the loss ??? The most unreassuring implications of your post is that you implicitly oppose any advance over quantum mechanics for particles in deep mutual entanglement, despite the shameful, century-old failure by quantum mechanics to represent nuclear data. Santilli hadronic mechanics has indeed achieved the first and I believe the only - to date - exact representation of nuclear spins, magnetic moments and other data in the true ground state of isolate nuclei. Your skepticism implies that we should keep the old uncertainties for nuclear structures and not seek better a representation of nuclear data. I hope for your own sake you are "not" aware of the implications of such a view for nuclear fusions etc.
Post 47
Can anybody indicate the representation via equations of at least one of Goedel's theorems? I could find none, as a result of which said theorems are epistemological at best. Hence, I understand and support Prof. Santilli's silence on them in his three proofs of the EPR argument to keep a distance from senseless and endless semantics on names.
Post 48
Prof. Santilli, could you please elaborate on the physical meaning of the isotopic element and its functional dependence?
Post 49
I believe that Post 39 and his friend 45 belong to the organized interests initiated by Bohr opposing any surpassing of QM for their pockets.
Post 50
Hello Post 48, thanks for the best question I received of lately. Recall that QM is a Hamiltonian theory which means that a system can be represented by QM if and only if the system is representable via the Hamiltonian H = p^2/2m + V(r). In my view, the biggest insufficiency of QM in nuclear physics at large and nuclear fusions in particular, is the impossible admission of an explicit and concrete representation of strong interactions due to their non-Hamiltonian character created, in nuclear physics, by the mutual penetration/entanglement of the charge distributions of protons and neutrons in a nuclear structure established by nuclear data. For this reason, I introduced the isotopy ATB of the associative product AB of QM so that electromagnetic (and part of the strong, such as the exchange) interactions are represented by the Hamiltonian H while the isotopic element T represents strong interactions in their most general possible non-linear, non-local and non-Hamiltonian form. In regard to the functional dependence of the isotopic element T, I assumed:
1) In its simplest possible form, T must have the exponential structure,
(1) T = exp X(....)
because such a form is the best for a smooth recovering of QM via the limit
(2) Lim T_{X -->0} = I.
2) In order for strong interactions to be attractive, the function X(...) has to be negative definite,
(3) T = exp [ - F(....)], ~~ F > 0.
3) F(...) is non-Hamiltonian by basic conception. Its primary functional dependence (again, in this simplest possible case) has to be in the wavefunction \psi(r) as a condition to represent the non-linearity of strong interactions (which is necessary for deep mutual penetration/entanglement). The non-locality of the strong interactions (also necessary for wave-overlapping/entanglement), joint with condition (2), restrict the simplest possible dependence of the isotopic element to the form (careful, when projected in our Euclidean space and not in isospace)
(4) T = exp{ - f(....) \int \psi^\dagger(r) \psi(r) d^3r}, ~~ f(...) > 0
which form assures that, when the wave overlapping/entanglement is insignificant, one recovers QM smoothly, identically and uniquely.
4) The verification of the last statement by Einstein, Podolsky and Rosen in their 1935 paper that "the wavefunction of quantum mechanics cannot represent the entire physical reality," requires that f(...) be also dependent on wavefunctions, by reaching in this way in the expression
(5) T = K exp{ - f(\psi. \psi*, ....) \int \psi^\dagger(r) \psi(r) d^3r}, K > 0, f(...) > 0
where: \psi is the QM wavefunction; \psi* is the "completed" wavefunction of HM; "..." refers to a number of additional functional dependences, when needed, on the density \mu, temperature \tau, frequency \vu, particle mutual distance d, local energy E, etc.; and the factor K may also have the most general possible dependence, provided that K = I when the particles are no longer appreciably entangled (e.g., non-spherical shapes become the perfect sphere with radius 1 for isolated particles in vacuum), see Eq. (4.7), page 170 of the monograph
http://www.santilli-foundation.org/docs/Santilli-113.pdf (formulated for the isounit I* = 1/T) and related Chapter 4 where one can see the achievement of the first attractive force between identical electrons in valence bonds, with related industrial applications for clean combustion of fossil fuels, see, e.g.,
www.hadronictechnologies.com. The above conception of non-Hamiltonian interactions realized with Isotopic element (5) has additionally allowed the first exact representation of "all" characteristics of the deuteron (not in a combination of excited states as done in QM to represent the spin 1, but) for the true ground state, see Section 2.7 of
http://eprdebates.org/docs/epr-review-iii.pdf that, in turn, allowed the conception of the conception of new nuclear fusions between natural, positively charged nuclei and negatively charged synthesized nuclei to avoid the enormous Coulomb barrier that has prevented the achievement to date of industrially viable clean nuclear energies. Regards, Ruggero.
Post 51
Thank you Prof. Santilli. To my understanding the isotopic element T can only have values between 1 (recovering of QM and zero (recovering of Einstein's full determinism)?
Post 52
Yes.<.p>
Post 53
Dear Sir post 47. I think you misunderstand me!
First, if you read my post 33, you will see that I am fully agree with
you about Santilli Hadronic Mechanics, which Prof Santilli has
recognized, see post 38.
2nd, thank you for the correction lose->loss.
3rd, We discuss science and nothing else, open mid is my home.
4th, now my point in post 45 is that: we do not know exactly whether
the nature for itself deterministic or not, this needs a final theory!,
we try to describe the nature by models in the spirit of Stepfen
Hawking, see post 33.
I presented my example about atom-apparatus to discuss the conditions
for the validity (my view) of the claim of Santilli the loss the
UNCERTAINTY.
We mankind when we measure the nature we test the validity of our
models. The extraction of information express the fact that we
transform the nature behavior to our consciousness.
We have to extract the information by apparatus and T->0 is achieved
by the condition that apparatus and the atom become close that mutual
penetration is large enough. Under this condition the atom and the
apparatus become (closed) one-system, and we can not gain any
information from (now becomes) is a closed-one-apparatus-atom system.
This sets some limitation on the claim of Santilli of the loss of
UNCERTAINTY, in my view. It is a simple Gedanken-Experiment.
Post 54
Post 53, please accept my apologies for misinterpreting your comments. Your comments regarding "limitations" on Santilli's proofs of the EPR argument are definitely valid and worth discussing. However, allow me to suggest that we should first discuss what is "Einstein isodeterminism" per Santilli's definition in his papers, and then pass to their limitations. This is recommendable because said proofs are mathematical. As stated by Santilli himself, their physical interpretation is essentially unknown at this writing. Also, their experimental verification requires "direct measurements under strong interactions", namely, a technology that does not exist in my knowledge at this moment.
Sorry again for my misinterpretation.
Post 55
I feel I should disagree with Post 53 in his view that Santilli's isodeterminism is purely mathematical. In the event that is the whole story, Heisenberg's uncertainties are purely mathematical because the former is constructed via an isotopy/axiom-preserving map of the latter. In reality:
Heisenberg's uncertainties were formulated for particles under electromagnetic interactions (because derivable from a potential), while,
Santilli's isodeterminism was formulated for strong interactions (because of contact non-Hamiltonain character). Hence there is a lot of underlying physics including industrial equipment based on it
The main issue is how to test Santilli's isodeterminism? I agree here with Post 54 because the tests require measurements under strong interactions, and that's not a cut of tea. However, it should be recalled that the first test here needed was proposed beginning with the title of Santilli's first paper introducing the words "hadronic mechanics",
R. M. Santilli, "Need of subjecting to an experimental verification the validity within a hadron of Pauli
exclusion principle," Hadronic J. Vol. 1, 574-901 (1978),
http://www.santilli-foundation.org/docs/santilli-73.pdf
Since that paper is 327 page long, I would appreciate whether Prof. santilli can tell us the main gist. We can then look for alternatives.
Post 56
Dear Post 55, thank you, it's okay no problem.
The limitation here means that the loss of UNCERTAINTY is limited to very extreme conditions. And one may ask under such conditions what about all physical laws. I must admit that I am not familiar with strong interaction, I should learn about it first.
Post 57
Post 56, I assume you know well QM. But then allow me to suggest that you study HM and its experimental verifications before entering into epistemological aspects related to "limitations." You will see that quantum equations and related laws (not just names) are replaced by covering hadronic equations and related laws.
Post 58
ELEMENTARY REVIEW OF RECENT STUDIES ON EINSTEIN'S DETERMINISM
Dear Post 55, thank you your request for me to provide an introduction to the experimental evidence supporting recent studies on Einstein's determinism. I confess that I hesitated to answer due to the limitations of the html format for equations, as well as for the technical character of the topic which requires a knowledge of at least the references of the announcement of our recent teleconference in the field [1], which references are reproduced below for convenience and are assumed to be known. The understanding of my elementary review also requires a knowledge of the lectures delivered at said teleconference [2].
1. Uncertainties for point-like particles.
We assume a knowledge that quantum mechanics can only represent point-like particles in vacuum (exterior dynamical problems) due to the sole possible definition of potentials, Laplacians, etc at isolated points.
Assume: a conventional Hilbert space H over the field of complex numbers C with states |ψ(t, r)> (where r is the Euclidean coordinate); normalization
(1) <ψ| | ψ> = 1;
and quantum mechanical realization of the linear momentum
(3) p |ψ > = - i ℏ ∂r |ψ >.
The familiar Heisenberg's representation then follows
(3) i dA/dt = [A, H] = AH - HA,
(4) [r, p ] = i ℏ , [r, r] = [p, p] = 0.
A well known procedure then yields Heisenberg's uncertainties for point-particles
(5) Δ r Δ p ≥ (1/2) | <ψ | [r, p] |ψ> | = ℏ /2
2. Experimental verifications of uncertainties for point-particles.
I personally believe in uncertainties (5) for point particles because of the clear experimental, verifications of Heisenberg's basic equations (3) and (4) for the hydrogen atoms and other exterior dynamical systems. These verifications are at times called indirect experimental verifications of quantum uncertainties (5). In fact, it is easy to prove that, in the event Eqs. (3) (4) are not verified experimentally, uncertainties (5) are invalid. Needless to say, in one century of repeated studies, there are also a number of direct experimental verification of quantum uncertainties (5), namely, verification with direct measurements of uncertainties (5) for exterior dynamical problems, such as the excellent experiments by Prof. Gerald Eigen (view his lecture in list [2]), and experiments quoted therein.
3. Isodeterminism for extended particles.
We assume a knowledge of isomathematics (Tutoring Lecture I of Ref. [2]) and its characterization of the isotopic branch of hadronic mechanics for the representation of extended particles in continuous mutual penetration/entanglement (Interior dynamical problems) [12] [13]. Assume the axiom-preserving/isotopic lifting/"completion" of "all" quantum mechanical products AB between arbitrary quantities A, B into the isoproduct
(6) A*B = ATB, T > 0,
where the isotopic element T represents extended particles in interior dynamical conditions and their ensuing non-linear, non-local and non-potential interactions (please look at Post 50 for the positive-definiteness of T > 0). Then, the isounit of the theory is given by
(7) I' = I'(r, p, ψ, ...) = 1/T > 0, I' * A = A * I' = A
Assume the iso-Hilbert isospace H' over the isofield C' of isocomplex isonumbers n' = n I' with isostates |ψ'(t, r')> (where t' = t for simplicity and r' = r I' ∈ C' represents, this time, a volume); isonormalization
(8) <ψ | * | ψ> = <ψ | T | ψ> = T ,
where one should note the necessity of the above isorenormalization (instead of <ψ | * | ψ> = <ψ | T | ψ> = I' ) since T can be a constant as a particular case; and the realization of the isolinear isomomentum of hadronic mechanics via the isodifferential calculus
(9) p'* | ψ'(t, r') > = - i ∂'r' |ψ' (t, r')> = - i I' ∂r' |ψ'(t, r') >,
where the upper dash represents quantities in H.
The repetition of the derivation of Eqs. (3, 4) under isotopy then yields the iso-Heisenberg isorepresentation[13]
(10) i d'A/d't = [A, H]' = ATH - HTA,
(11) [r, p ]' = i I';, [r, r]' = [p, p]' = 0.
Note that hadronic mechanics recovers quantum mechanics uniquely, unambiguously and entirely at the limit T = 1 (Post 50).
As it is well known, N. Bohr [4] strongly opposed to his death Einstein's desire for a return to classical determinism. For the case of two point-like particles with spin 1/2 in vacuum represented by quantum mechanics (qm), Bohr's view was supported by J. S. Bell [5] who computed an inequality of the type
(12)
Dqm ≤ 2,
whose value prevented the existence of classical counterparts, thus preventing a realization of Einstein's determinism (see the vast literature in Ref. [6]).
First verification of the EPR argument [3]. The following two-dimensional realization of the isotopic element T for particles with spin 1/2 , first introduced in Ref. [7],
(12) T = Diag. (1/λ, λ), Det T = 1
provides an explicit and concrete realization of Bohm's hidden variables. [5]. The repetition of of the derivation of Bell's inequality [5] via hadronic mechanics (hm) for the representation of two expended particles with spin 1/2 in continuous overlapping/entanglement and hidden variables λ and μ, respectively, yields the expression [7]
(13)
Dhm = (1/2)(λ μ-1 + μ λ-1) Dqm
whose large factor implies that the explicit and concrete realization of hidden variables permitted by hadronic mechanics establishes the existence of classical counterparts for systems of extended particles with spin 1/2 in
interior dynamical conditions, by therefore identifying conditions under which Einstein's determinism is possible (see Ref. [7] for the identification if specific classical images).
Second verification of the EPR argument [3]. The step by step isotopy of the derivation of uncertainties (5) yields the isodeterminism for extended particles [8]
(14) Δ' r Δ' p = (1/2) | <ψ' | * [r, p] * |ψ'> | = T/2
which isodeterminism progressively and smoothly connects Heisenberg's uncertainties (5) occurring for T = 1 to Einstein's full determinism occurring for T = 0 at the extreme densities of Schwartzchild's horizon [8]
(15)
T = 1 / (1 - 2M/r) --> r -->0 = 0,
with intermediate conditions depending on the density of the deep entanglement of particles.
Third verification of the EPR argument [3]. The proof of the last statement of Ref. [3], that "quantum mechanical wavefunctions cannot represent the entire physical [and chemical] reality," was done in monograph [15] and Ref. [11], Section 2.8, with the first known identification of an attractive force between the two identical electrons in valence bonds with ensuing exact representation of molecular data. This proof is not reviewed here for brevity. We merely note that hadronic laws (13) (14) are solely possible under the "completion" of quantum mechanical wavefunctions for non-linear, non
-local and non-potential interactions. The achievement of an attractive force between identical valence electrons is then consequential.
4. Indirect Experimental verifications of isodeterminism.
In my view, as it is the case for uncertainties (5), the most important verifications of isodeterminism (13) are given by the experimental verifications of the basic laws of hadronic mechanics, the iso-Heisenberg isorepresentation and its isounitarily isoequivalent iso-Schr\"oringer isorepresentation [13], since the latter uniquely and unambiguously imply the former.
4.1. Verification via the synthesis of the neutron from the hydrogen. The neutron is 0.782 MeV heavier then the sum of the masses of the proton and the electron, under which conditions no representation via quantum mechanics is possible for various technical reasons. Following decades of research, the iso-Schr\"odinger isorepresentation has permitted the representation of the totality of the characteristics of the neutron in its synthesis from the hydrogen at the non-relativistic and relativistic levels, as well as the industrial construction and sale of an equipment producing neutrons on demand from the hydrogen in the desired direction, energy and flux (see Ref. [15], Vol. IV, the first lecture by Prof. S. Beghella-Bartoli in Ref. [2] and independent review [18]).
4.2. Verification with the characteristics of the deuteron. The basic dynamical laws of hadronic mechanics have additionally permitted the first known exact representation of all characteristics of the deuteron thanks to the first known representation of strong interactions via the isotopic element T (see Section 2.7 of Ref. [11]).
4.3. Verification via nuclear magnetic moments.
Recall that, in one century of efforts, quantum mechanics has been unable to achieve an exact representation of the magnetic moment of the smallest nucleus, the deuteron, with embarrassing deviations of the predictions of the theory from experimental data for heavier nuclei. The first proof [7] of the EPR argument [3] was applied in the same paper [7] for the first known numerically exact representation of nuclear magnetic moments because the extended character of particles implies their deformability under strong interactions, thus providing the missing anomalous contribution for exact representations (see also Section 2.7 of Ref. [11]).
4.4. Verifications via nuclear spins.. Recall that, also in one century of research, quantum mechanics has been unable to represent the spin J = 1 of the the deuteron in its ground state since that would require, for stability, a singlet coupling of protons and neutron in which case the spin would be null, J = 0. This occurrence has forced orthodox physicists to represent the spin J =1 via a combination of excited orbital states against the incontrovertible experimental evidence that an isolated deuteron is in its ground state with J = 1. The iso-Heisenberg isorepresentation and the related regular isotopies of the SU(2) spin symmetry [10] have permitted the achievement of an exact representation of the spin of nuclei in their actual ground state [14].
4.5. Representation via the anomalous behavior of the mean life of unstable hadrons with speed.
The admission that particles have an extended wavepacket implies that hadrons are hyperdense media caused by the total mutual penetration/entanglement of their constituents. The resulting internal, non-linear, non-local and non-Hamiltonian interactions can manifest themselves in the outside via the experimentally measured deviation from quantum predictions of the mean life of unstable hadrons with energy from 0 to 100 GeV. By contrast, these deviations are exactly represented by relativistic hadronic mechanics (see Volume IV of Refs. [15]).
4.6. Verifications via the Bose-Einstein correlation. It is generally believed at orthodox institutions that relativistic quantum mechanics is exactly verified by the Bose Einstein correlation. However, the fit of experimental data requires four arbitrary parameters (called "caoticity parameters"?), whose introduction from basic axioms is impossible since the quantum mechanical expectation value of the
Hamiltonian <ψ | H |ψ> for the two-point correlation functions is only two-dimensional. By contrast, the use of relativistic hadronic mechanics has permitted the exact representation of the experimental data from first unadulterated principles for the two-point correlation function thanks to the isoexpectation values <ψ | * H * |ψ> = <ψ | T H T |ψ> which provide experimental values of the shape, dimension and density of the proton-antiproton fireball (see Vol. IV of Ref. [15]).
4.7. Experimental verifications via molecular data. As well known, quantum mechanics is exactly valid for the structure of one hydrogen atom, while failing to achieve an exact representation of two hydrogen atoms bonded into the molecule H-H, since the quantum representation misses the rather large amount of 941 kcal/mole in the representation of the H2 binding energy. By acknowledging the historical value of the quantum chemical valence, I achieved its "completion " with an attractive force between the identical valence electrons, that permitted the representation of binding energy of the hydrogen and water molecules numerically exact to the desired decimal value (see Refs. [11], [15] Vol. V, and [16]).
A number of additional experimental verifications exist via the use if the irregular isosymmetries for extended particles in interior conditions (see Ref. [10], [13], and Vol. III of Ref. [15]), but they cannot be reviewed in this rudimentary presentation for brevity. However, to prevent major misrepresentations, it is necessary to recall that, by no means, "particles in interior conditions" (electron, proton, neutron, etc.) are the same as the corresponding "particles in exterior condition," because the latter particles are unitary irreducible representations of the Lorentz-Poincare' symmetry, while the former particles are isounitary isoirreducible isorepresentation of the covering Lorentz-Poincare'-Santilli isosymmetry called isoparticles. The main difference is due to the fact that non-Hamiltonian interactions represented with the isotopic element T cause renormalizations of intrinsic characteristics (mass, charge, magnetic moment, etc., first identified in Eq. (5.1.36), page 841. Ref. [17] of 1978), without which none of experimental verifications 4.1 to 4.7 would be possible.
5. Direct experimental verifications of isodeterminism.
Post 55 has identified what appears to be the expected, most important, yet most, difficult, direct verification of isodeterminism, that via the confirmation or disproof of Pauli's exclusion principle under strong interactions. In essence, alongside the isodeterminism, the mutations of intrinsic characteristics of particles increase with the increase of the density of the hadronic media. In particular, the spin 1/2 of electrons and protons does not need to be mutated for the structure of the neutron and of light stable nuclei. However, hadronic mechanics predicts that, at the extremely high energies of ongoing particle collisions at CERN, FERMILAB, DESY and other laboratories, the intrinsic angular momentum of particles cannot remain the same as when in vacuum due to surrounding resistive forces, thus implying the prediction (made in 1978 [17]) that Pauli's exclusion principle cannot be verified in the extremely high density scattering regions. Thanks for the interest and best wishes. R. M. Santilli
REFERENCES
[1] 2020 International Teleconference on Einstein's Determinism
[2] Lectures delivered at the 2020 teleconference
[3] A. Einstein, B. Podolsky , and N. Rosen, ``Can quantum-mechanical description of physical reality be considered complete?,'' Phys. Rev., vol.~47 , p. 777 (1935),
http://www.eprdebates.org/docs/epr-argument.pdf
[4] N. Bohr, ``Can quantum mechanical description of physical reality be considered complete?" Phys. Rev. Vol. 48, p. 696 (1935),
http://www.informationphilosopher.com/solutions/scientists/bohr\-/EPRBohr.pdf
[5] J. S. Bell: ``On the Einstein Podolsky Rosen paradox" Physics Vol. 1, 195 (1964),
https://cds.cern.ch/record/111654/files/vol1p195-200_001.pdf
[6] Stanford Encyclopedia of Philosophy, ``Bell's Theorem" (2019),
https://plato.stanford.edu/entries/bell-theorem
[7] R. M. Santilli, ``Isorepresentation of the Lie-isotopic SU(2) Algebra with Application to Nuclear Physics and Local Realism," Acta Applicandae Mathematicae Vol. 50, 177 (1998),
http://www.eprdebates.org/docs/epr-paper-i.pdf
[8] R. M. Santilli, ``Studies on the classical determinism predicted by A. Einstein, B. Podolsky and N. Rosen," Ratio Mathematica Volume 37, pages 5-23 (2019),
http://www.eprdebates.org/docs/epr-paper-ii.pdf
[9] R.M. Santilli, ``Studies on A. Einstein, B. Podolsky, and N. Rosen prediction that quantum mechanics is not a complete theory, I: Basic methods,"
Ratio Mathematica Volume 38, pp. 5-69, 2020,
http://eprdebates.org/docs/epr-review-i.pdf
[10] R.M. Santilli, ``Studies on A. Einstein, B. Podolsky, and N. Rosen prediction that quantum mechanics is not a complete theory, II: Apparent proof of the EPR argument,"
Ratio Mathematica Volume 38, pp. 71-138, 2020,
http://eprdebates.org/docs/epr-review-ii.pdf
[11] R.M. Santilli, ``Studies on A. Einstein, B. Podolsky, and N. Rosen prediction that quantum mechanics is not a complete theory, III: Illustrative examples and applications,"
Ratio Mathematica Volume 38, pp. 139-222, 2020,
http://eprdebates.org/docs/epr-review-iii.pdf
[12] R. M. Santilli, Elements of Hadronic Mechanics,
Ukraine Academy of Sciences, Kiev,
Volume I (1995), Mathematical Foundations,
http://www.santilli-foundation.org/docs/Santilli-300.pdf
[13] R. M. Santilli, Elements of Hadronic Mechanics,
Ukraine Academy of Sciences, Kiev,
Volume II (1994), Theoretical Foundations,
http://www.santilli-foundation.org/docs/Santilli-301.pdf
[14] R. M. Santilli, Elements of Hadronic Mechanics, Ukraine Academy of
Sciences, Kiev,
Volume III (2016), Experimental verifications,
http://www.santilli-foundation.org/docs/elements-hadronic-mechanics-iii.compressed.pdf
[15] R. M. Santilli, Hadronic Mathematics, Mechanics and Chemistry,
Volumes I to V, International Academic Press, (2008),
http://www.i-b-r.org/Hadronic-Mechanics.htm
[16] R. M. Santilli, Foundations of Hadronic Chemistry, with
Applications to New Clean Energies and Fuels, Kluwer Academic
Publishers (2001),
http://www.santilli-foundation.org/docs/Santilli-113.pdf
Russian translation by A. K. Aringazin,
http://i-b-r.org/docs/Santilli-Hadronic-Chemistry.pdf
[17] R. M. Santilli, "Need of subjecting to an experimental verification the validity within a hadron of Pauli
exclusion principle," Hadronic J. Vol. 1, 574-901 (1978),
http://www.santilli-foundation.org/docs/santilli-73.pdf
[18] I. Gandzha and J. Kadeisvili, New Sciences for a New Era, Sankata Printing Press, Nepal (2011),
http://www.santilli-foundation.org/docs/RMS.pdf
Post 59
Prof. Santilli! following your magnificent Post 58, in addition to the great honor reviewed in Post 19, I feel obliged to reproduce the words expressed by the famous British historian Sir Karl Popper in his inspiring book Schism in Physics, Cambridge University Press (1982) on Sir R. M. Santilli
(http://santilli-foundation.org/santilli-nobel-nominations.html):
"I have mentioned Santilli, and I should
like to say that he-one who belongs to a new generation - seems to me to
move on a different path. Far be it from me to belittle the giants who
founded quantum mechanics under the leadership of Planck, Einstein,
Bohr, Born, Heisenberg, de Broglie, Schrodinger, and Dirac. Santilli too
makes it very clear how greatly he appreciates the work of these men. But
in his approach he distinguishes the region of the 'arena of incontrovertible
applicability' of quantum mechanics (he calls it 'atomic mechanics') from
nuclear mechanics and hadronics, and his most fascinating arguments in
support of the view that quantum mechanics should not, without new tests,
be regarded as valid in nuclear and hadronic physics, seem to me to
augur a return to sanity: to that realism and objectivism for which Einstein
stood, and which had been abandoned by those two very great physicists,
Heisenberg and Bohr."
Post 60
Prof. Santilli, I have initiated the best study I can of your works and would appreciate your help in understanding steps that for you are perhaps trivial. The first one is the inapplicability of Scrhoedinger equation for the bound state of a proton and an electron at 10^{-13} cm. I can get nothing that makes physical sense despite their mutual "astronomical Coulomb attraction" you have mentioned. Thanks.
Post 61
Hi Post 60. I think you got it the way you put it: by using QM you get nothing that makes physical sense for the fusion of a proton and an electron into the neutron in the core of stars despite their huge attraction. I did study Prof. Santilli's long journey and I believe you should do the same. FIRSTLY, you should understand how hadronic mechanics makes full sense for the synthesis of particles with excess mass by studying the derivation of all (note, all) features of the π0 in its synthesis from the positronium despite about 132 MeV excess mass (!). This is best done in Table 5.2, page 849 of Prof. Santilli's originating paper http://www.santilli-foundation.org/docs/santilli-73.pdf. None of the various subsequent reviews come even close to that presentation. SECONDLY, you should understand how hadronic mechanics achieved a representation of all (note, all) features of the neutron in its synthesis from the proton and the electron at the non-relativistic level. Again, this is best done in Prof. Santilli's originating paper with no better second
http://www.santilli-foundation.org/docs/Santilli-21.pdf. THIRDLY, to understand the relativistic treatment you got to study first Santilli's isosymmetries, particularly the Lorentz-Poincare'-Santilli isosymmetry, see the review http://eprdebates.org/docs/epr-review-ii.pdf. After you got such a knowledge, then you should study, again, Prof. Santilli's original relativistic representation of all (note, all) features of the neutron in its synthesis in the core of stars with no better presentation on record in my view http://www.santilli-foundation.org/docs/Santilli-18.pdf. But then you may ask why bother? To see the answer look around in academia. There is nothing besides rotten postures in opposing new discoveries to protect their turf. The sole scientific novelty around is that by Prof. Santilli. Therefore, sooner or later our Feds will finally understand that and test Santilli's hyperfusion between synthesized negatively charged deuterons and natural deuterons into helium, D(-1, 2, 1_up) + D(1, 2, 1_\down) = He(2,
4, 0) + 2e http://eprdebates.org/docs/epr-review-iii.pdf.At that point you will be the expert because orthodox physicists will only blab by comparison.
Post 62
Prof. Santilli, attending your lectures at EPR-2020 conference on the completion of QM as suggested by Einstien, Rosen and Podolsky was a great experience. Your arguments are foolproof and deserve to be acknowledged by the scientific community. You have opened new vistas for theoretical and experimental Physics as well as in the fields of Mathematics and Chemistry. Your work is epoch making and deserves to be awarded by the Nobel prize. Your dedication and devotion to the subject is unparalleled. In fact, your work is going to affect classical thinking giving way to a new way of thinking which is most modern.
Post 63
Dear Post 62, I believe I have provided ample proof that, when I was at BU, MIT, Harvard University, ICTP, JINR and other institutions I never looked for an academic career and solely searched for new scientific knowledge, at times against the view of my distinguished colleagues, because I knew then and know now the pressing need of new knowledge for the otherwise unsolvable, increasingly alarming environmental problems such as recycling nuclear waste, clean nuclear energies, clean combustion of fossil fuels et al. Thank you, Post 62, your nice words provide a sense to all these efforts for so many years. Best wishes, Ruggero Santilli
Post 64
Prof. Santilli, your recent release on Einstein's isodeterminism is brilliant. I am developing a deeply complimentary theory, and have a the following
Question: Would the singlet coupling of a negative energy pseudophoton (with its implied reversal of properties within this system) and a positive energy photon add to spin two, or spin zero?
Thanks!
Post 65
Dear Post 64, thanks for the intriguing and important question. To our knowledge, the pseudoproton is made up of ordinary matter, thus existing in our spacetime, because synthesized by our Directional Neutron Source via the compression of an electron inside a neutron. As such, the sole new features of the pseudoproton with respect to the proton are the reversal of the sign of the charge and of the direction of the magnetic moment. Under these conditions, a singlet state of a pseudoproton and a proton has spin zero. BUT, this view is based on the central feature of the synthesis of the neutron (which persists in the synthesis of the pseudoproton), namely, the compression of a particle with spin 1/2, the electron, inside an hyperdense particle with spin 1/2, the proton (the neutron), yields the total angular momentum 1/2 of the neutron (pseudoproton) because of the constrained angular momentum of the electron within a hyperdense hadron with spin 1/2. This feature is fully represented by the irregular SU(2) spin symmetry (for its treatment, see Section 3 of the paper http://eprdebates.org/docs/epr-review-iii.pdf, and for its application to neutron and pseudoproton, see Section 2.6 of http://eprdebates.org/docs/epr-review-ii.pdf). The corresponding important question of the total spin of a bound state of a true antiproton (existing in its isodual spacetime over isodual numeric fields) and a proton (existing in our spacetime over ordinary numeric fields) was raised by Evans Boney during the discussions of our recent International Teleconference on Einstein's Determinism, but we do not know the answer at this writing due to basic aspects currently under investigation. Ruggero
Post 66
Prof. Santilli, please indicate the reason for which the total spin of coupled antiproton-proton pair is unsettled. Thanks.
Post 67
Prof. Santilli, The bound state of the particle and its antiparticle is indeed crucial to consider, and I would like to consider it a bit further. First let's note that there are bound states for positronium and muonium that are more accessible than the proposed antiprotonium (?)... and I would suggest Prof. Kaplan's work developing MAGE as very interesting and relevant (https://arxiv.org/abs/1802.01438 ). But on to the math. As Prof. Santilli notes, there is indeed the question of 0 or 2 total spin (responding to Post 64), but let's examine further ramifications of this concern. For instance, gravitational mass. The isodual particle has mass -M, and the particle has mass M, when projected into the spacetime we live in. The usual two-body treatment would suggest breaking this into a center of mass and reduced mass, each of which has the sort of concern Prof. Santilli mentions.
Post 68
Dear Posts 66 and 67, your questions are deeply related and quite important indeed. Unfortunately, html commands are limited and, therefore. my comments will be at best rudimentary. The only way I know is to start from the foundations to check them out in order not to be sorry later. Also, I can express below my personal view and be grateful to anybody who has strong counterarguments. "THE" starting point is the lack of "completeness", in my view, of charge conjugation
(1)
ψC(t, r) = - ψ† (t, r)
because it maps antiparticles in the spacetime and Hilbert space of particles, thus preventing the representation ofc matter-antimatter annihilation (since two positive masses cannot annihilate into light). For this reason, I "completed" charge conjugation into the isodual map, denoted with the upper index "d", which is also an anti-Hermitean map like charge conjugation [1],
(2)
ψd(t, r) =
- ψ†(- t†, - r†)
the main difference is that the isodual map must be applied to the totality of quantum mechanical quantities and all their operations You miss one isodual map and get an Italian minestrone. Despite its elementary character, the isodual map (2) has far reaching implications such as: the positive energy of particles is mapped into negative energy for antiparticles (Dirac 1929), thus allowing a quantitative representation of matter-antimatter annihilation; the Minkowskian spacetime is mapped into a new spacetime coexisting with our own; charge conjugation solely applies in a Hilbert space, while the isodual pam applies beginning at the classical level, with its application to a Hilbert space being a small particular case, thus rendering inevitable the study of the possible existence of antimatter galaxies; etc.To start addressing the issues raised by Posts 66 and 67, let us recall from Ref. [1] the maps of the quantum mechanical eigenvalue equation for spin and energy into their isodual images which have not raised controversies to date (below we assume E>0)
(3)
J3 × ψ(t, r) = +/- ½ ψ(t, r) - - > J3d ×d ψd(td, rd) = (-/+ ½) (- ×) [- ψ†(-t, - r)]
(4)
H(r, p) × ψ(t, r) = E × ψ(t, r) -->
--> Hd(rd, pd) ×d ψd(td, rd) = (- H) (-×) [- ψ†(-t, -r)] = - H(r, p) × ψ†(- t, - r) =
= Ed ×d ψd(td, rd) = - E × ψ†(-t, -r)
Consequently, the spin and energy reverse their sign when represented in their isodual space as I believe we all agree. The open issues raised by Posts 66 and 67 occur in the projection of the isodual values into our spacetime. The projection adopted in Ref. [1] for reasons indicated below is given by
(5)
J3d×d ψ(t, r) = +/- ½ ψ(t, r)
(6)
Hd ×d ψ(t, r)] = E × ψ(t, r)
namely, the eigenvalues of the isodual quantities have to be computed on conventional Hilbert states because they represent our world.
It then follows that the projection in our Hilbert space of isodual spin an d energy coincide with conventional values. In this case, a particle-antiparticle state in singlet coupling has spin zero in our space as well as in the isodual space, while the energy of the positronium is positive in our space and negative in its isodual (for more details please inspect Section 2.3.14 'Isoselfdual bound states, page 131, Ref. [1]]).
Question: so where is the controversy? Answer: in Ref. [1], solely for isoselfdual states (see below) I assume projections of the type
(7)
Hd ×d ψ = (-H) (-×) &psi = H × ψ
while others assume the different projection
(8)
Hd × ψ = (-H) × &psi = - H × ψ
namely, they do not subject the product × to the isodual map, thus ending up with opposite results.
The reasons underlying my assumption are several. To begin, the isodual theory must be formulated on isodual numeric fields, namely, numbers with a negative unit which means that negative values are measured with negative unit. But then, the projection in our space of a negative isodual quantitive measured with negative unit has to be positive for consistency. This is a crucial assumption for the consistency of any theory on antimatter because NEGATIVE ENERGIES IN OUR SPACETIME VIOLATE CAUSALITY (DIRAC 1928), The only way I know to solve this basic flaw is via isodual numbers because a negative energy referred to negative units is as causal as a positive energy referred to positive units, and the same goes for time, etc.
extended particles and antiparticle systems that cannot be reviewed here (see Ref. [1]). In a nutshell, when isolated in vacuum, particles and antiparticle have everything opposite to each other. Annihilation then follows prior to any projection in one space or another. When in a state the deep entanglement needed for a bound state, the notions of "electron" and "positrons" as commonly understood are gone in favor of isoparticles much similar to two identical electrons turning their huge Coulomb repulsion into a huge attraction in their valence bond. To my understanding, the positive energy of the positronium is a result of the mutation of the structure of both particles and antiparticles. This is essentially what I know. Again, I gratefully invite criticisms of technical character, by keeping in mind that I am not an expert of epistemological studies. Cheers Ruggero Santilli
[1] R. M. Santilli, Isodual Theory of Antimatter with Applications to Antigravity, Grand
Unifications and Cosmology, Springer (2006).
http://www.santilli-foundation.org/docs/santilli-79.pdf
www.santilli-foundation.org/docs/santilli-79.pdf
Post 69
Prof. Santilli, thank you for your detailed review on your isodual theory of antimatter. I agree with your equations (5) and (6) because the product ×d is the base product of the isodual theory beginning with the product of the isodual numbers and, consequentially it must be kept in the projection in our space. Only the wavefunction should change fform the isodual form to our form . The implications are big and exciting. Congrats!
Post 70
There seems to be a contradiction in Santilli's Post 68. On one side he says that negative masses are needed for a representation of matter-antimatter annihilation. On the other side he says that the projection in our space of a negative mass measured with negative unit is positive. Hence, the contradiction...
Post 71
No contradiction if you treat the problem with equations rather than words. Matter-antimatter annihilation occur at contact. Hence, there is no need for any projection in our space and the representation of matter-antimatter annihilation follows. By contrast, the positronium is a bound state in our spacetime, in which case a projection is necessary for a small yet finite lifetime.
Post 72
I would like to thank the authors of the preceding posts for their interest in the intriguing issue of the mass of the positronium. Unfortunately, I see in some post the continued oblivion for Dirac's proof that a negative mass is our spacetime violates causality and, as such, it cannot exist. In fact, Dirac's causality problem - that lead to his conception of the 'hole theory' - can be applied almost identically to a negative mass for the positron in the positronium. Another unfortunate aspect that appears to be ignored is the lack of referral of negative masses to negative units as the only known way (in case there are others please let me know, thanks) to avoid violation of causality with negative masses in our spacetime. In conclusion, the only way to write correctly the reduced mass of the positronium in MeV units in the isodual theory of antimatter (and not in other theories) is given by
(1)
μ = m/ + MeV × - m/ - MeV / ( m/ + MeV - m/ - MeV ) = m MeV/2 = 0. 255 MeV
Again, colleagues are free and welcome to use any different theory, but then please do not mention the isodual theory of antimatter. Sincerely. RMS
Post 73
I would ask those mentioned who are still in consideration of the query I raised in question number 64 that was answered in number 65 to consider the source of the coupled photon and anti-photon as extending simultaneously from the T field from positive and negative energies as specified in
P. M. Jack; 2003, Physical Space as a Quaternion Structure, 1;
Maxwell equations. A Brief Note, arXiv:math-ph/0307038v1 and Dunning-Davies, J. and Norman, R.L. (2020) Deductions from
the Quaternion Form of MaxwellÕs Electromagnetic
Equations. Journal of Modern
Physics, 11, 1361-1371
https://doi.org/10.4236/jmp.2020.119085
I believe we see the emergence of gravitons across the T field. There is a 7th scalar part to electromagnetic expressions with positive and negative energetic components associated with electrons and protons respectively. The effects are not only energetic but gravitational, see Richard Lawrence Norman and Jeremy Dunning-Davies, ?A Discussion of Unconventional Theories related
to Gravity: Energy, Plasmas and Propulsion, Parana Journal of Science and Education. Vol. 6, No. 4, 2020,
pp. 51-64.
https://doi.org/10.5281/zenodo.3880526
It is possible to draw some interesting theoretical possibilities out at this juncture.
To observe the larger mass of the proton with its negative and convergent energies, we may infer the attractive magnetic force is evidence of a mass associated negative energetic residual in its slight primacy over the repulsive magnetic force. Please think also of Brillouin and his notions of gravitation as extending from negative mass mentioned in the reference above. Hence, being composed of quantum of both energies, gravitons reduce by a similar residual quantity the energy between massive bodies, accounting for gravitational attraction, an idea first put forward by Maxwell, although without any mention of negative energy. Also, that residual must be accounted for in creating the neutron, then, implying perhaps, need for a positive binding energy and the neutrino/aetherino at .78MeV. The neutrino/aetherino could be needed to create a truly energy neutral neutron, which is at stable equilibrium.
Post 75
Post 70, please explain what is the T field? The field of the isotopic element T? The isodual theory of antimatter is based on a vacuum composed by the superposition of extremely high densities of positive and negative energies. Positive energies are needed for the synthesis of neutrons and negative energies are needed for the synthesis of anti-neutrons. Their only known representations is that via the isotopic element T. Is this in line with your thinking?
Post 726
EDITORIAL NOTE: This the replacement of Post 67 for apparently unauthorized editorial changes. by the author's request
bound state of the particle and its antiparticle is indeed crucial to consider, and I would like to consider it a bit further. First let's note that there are bound states for positronium and muonium that are more accessible than the proposed antiprotonium (?)... and I would suggest Prof. Kaplan's work developing MAGE as very interesting and relevant (https://arxiv.org/abs/1802.01438 ).
But on to the math. As Prof. Santilli notes, there is indeed the question of 0 or 2 total spin (responding to Post 64), but let's examine further ramifications of this concern. For instance, gravitational mass. The isodual particle has mass -M, and the particle has mass M, when projected into the spacetime we live in. The usual two-body treatment would suggest breaking this into a center of mass and reduced mass, each of which has the sort of concern Prof. Santilli mentions.
However, while the antiproton / isodual proton exists in the isodual space, we can always take its projection into our space, and indeed that's part of what's so valuable about the theory! So, for masses at least, I think the M_COM = M - M = 0, because the projection of the isodual mass into our space leads to repulsion, which must be continued even for bound states, which are not split between worlds, they exist fully in each. In this case, we would expect Muonium, Positronium, etc to float / have no gravitational mass.
But then, what of the reduced mass (which is now infinite / NAN)?! I'm afraid I don't know more than to say... that sure looks like a problem. Vibrational states with zero frequency? Fun to think about... but also proven wrong for Positronium already.
I think in the past I have attempted to parse the types of mass here... noting that the reduced mass is used in inertial/rest mass situations (so the masses all get absolute values) but the COM is used in gravitational situations, which seems ok, but maybe not fully convincing to someone who wasn't already ideologically committed to it as a means to an end.Ó I will add the additional questions in the future per your request, but please let me know when the work you mentioned discussing Lie-Admissible Lorentz symmetric algebras and neutrinoless double beta decay is posted.
Post 74
Unfortunately, I see no connection between Post 72 and the isodual theory of antimatter because the post continues to consider negative masses tacitly referred to positive unit, without acknowledging Dirac's violation of causality, without acknowledging the explicit opposing calculations of Posts 68 and equation (1) of 72, etc. Am I missing something or Post 73 is misses big?
Post 75
As far I am concerned, the acceptance of the isodual theory of antimatter implies a positive total mass of the positronium per Prof. Santilli's Eq. (1) of Post 72 and preceding Post 68. I do not understand the problem raised by Post 70 because the isodual map is equivalent to charge conjugation when formulated in a Hilbert space. The conjugation to antimatter used in Post 70H 'is' the conventional charge conjugation because referred to positive units. Hence, the use of the argument by Post 70 applied to standard charge conjugation leads to a null mass of the positronium which is known not to be true.
Post 76
In my view, referring negative/antimatter energies to positive units of our matter world is like referring positive/matter energies of our world to the negative units if the antimatter world with evident inconsistency.
Post 77
To Post 7.2. please explain how we know positronium does not have a null gravitational mass. The experiment has not been done to my knowledge. And since you've referenced charge, let's stay with that a second: does the isodual theory also think positronium has a slight positive charge? What part of the prior logic for masses fails for charges? To my eye it seems like we are using E=mc^2 to infer the mass from the energy, when that equation is not itself the end of the story (derived as it is from E^2=m^2c^4 norm at rest, without considering negative mass possibilities).
Post 78
Hello Post 77, thanks for your questions. They are all important and pertinent. To my understanding, the
isodual theory of antimatter
predicts the following features in a unique and unambiguous form, to such an extent that, in the event any one of them is disproved by clear and direct (not indirect) "experiments", the entire theory becomes inapplicable.
1. The total rest energy of the positronium is positive in our matter-space and negative ion the antimatter space (Eq. (1) of Post 72 and preceding reference).
2. Having a positive rest energy, the positronium has a non-null, although small gravitational mass.
3. The charge of the positronium can only be identically null because the positronium is isoselfdual ( invariant under isoduality).
4. The logic for the calculation of total masses and charges for isoselfdual states are the same.
5. E = mc^2 is exactly valid solely for point-masses in vacuum. For extended masses within physical media, such as for a pion in the core of a star, E = m c2 cannot be exactly valid for numerous reasons, such as the fact that the anisotropy of the medium caused by rotation of the star implies that observers at the equator and at the poles detect necessarily different values. This applies particularly for the energy equivalence of the mass of the positronium because its constituents are in condition of total mutual entanglement (necessary to create a bound state), thus being isoparticles, i.e., isoirreducible isounitary isorepresentations of the LPS isosymmetry, see Section 2 of http://eprdebates.org/docs/epr-review-ii.pdf. The second order iso-Casimir isoinvariant then yields the energy equivalence in the k-direction Ek = m c^2 nk2/ n42. Critical comments on my apparent proof of Einstein's determinism (Post 58 and references quoted therein) would be appreciated. R. M. Santilli
Post 79
CRITICISM OF SANTILLI'S PROOF OF EINSTEIN'S DETERMINISM.
I would like to praise Prof. Santilli for soliciting criticisms of his proofs of Einstein's determinism (Post 58 and related references) presented at the 2020 International Teleconference on Einstein's Determinism
http://eprdebates.org/epr-conference-2020.php
see the lectures and comments delivered at the teleconference
http://www.world-lecture-series.org/level-xii-epr-teleconference-2020.
Here is what I could gather in academic corridors (the references are those of Post 58):
CRITICISM 1. The Einstein-Podolsky-Rosen Argument [1] is "flawed because it does not account for the quantum nature of the observation by the sensor. Bell's theorem would later suggest that local hidden variables (a way for finding a complete description of reality) of certain types are impossible." https://en.wikipedia.org/wiki/Hidden-variable_theory
CRITICISM 2: Hidden variables have mathematical meaning and the same holds for Santilli's realization T = Diag. (1/λ, λ) of hidden variables via the isotopic element T of the isoproduct ATB [7].
CRITICISM 3. In the uncertainty relations Δ r Δ p ≥ ℏ /2, Planck's constant has the value h= 6.62607015 x 10- 34 J.s representing the smallest possible quantum action. In Santilli's isouncertainty relations Δ r Δ p = T/2,
comparatively smaller values of the isotopic element T do not have physical significance.
CRITICISM 4. The replacement of "≥ " in the uncertainty relations Δ r Δ p ≥ ℏ /2 with the equality in the isouncertainty relations
Δ r Δ p = T/2 voids the statistical character of quantum measurements https://en.wikipedia.org/wiki/Statistical_mechanics , with consequential unreliable experimental data
CRITICISM 5. Per his own admission, Santilli's isouncertainties only hold at mutual distances of particles of the order of 10-13 cm in the interior of strongly interacting systems such as nuclei. But then the nuclear center of mass follows quantum uncertainties, resulting in the recovering of quantum uncertainties for nuclear constituents.
Additional criticisms are not reported here because excessively biased.
Post 80
I would like to thank Post 79 for criticism of my apparent proofs of Einstein's determinism that have to be debated. I also welcome the quotation of Wikipedia's 'Articles' since they represent the view of the orthodox academic community and, consequently, of governmental funding agencies. In a nutshell, the view of the Wikipedia-academia
-governmental complex is a continuation of the dismissal, initiated by Niels Bohr in 1935, of Einstein's prediction that "quantum mechanics is not a complete theory," with the ensuing tacit assumption that quantum mechanics can represent all conceivably possible conditions existing in the universe. The schism in physics pointed out in 1978 by Sir Karl R. Popper (Post 59), and by numerous other scientists including myself, is essentially based on the acceptance of the exact validity of quantum mechanics for electromagnetic interactions between point-like particles, while considering quantum mechanics as an approximate theory for strong interactions between extended and entangled particles, with the ensuing need for a suitable "completion" of quantum mechanics for the interior of hadrons, nuclei and stars. The experimental evidence that prompted said schism is that, in about a century of studies and the use of large public funds, quantum mechanics has been unable to achieve an exact representation of
nuclear magnetic moments, nuclear spins, nuclear forces, nuclear stability, and other nuclear data. This caused the inability by quantum mechanics and therefore of quantum chemistry, also in about one century and the use of large public funds, of solving basic environmental needs, such as: the recycling of radioactive nuclear waste via their stimulated decay or other means; industrially viable controlled nuclear fusions; full combustion of fossil fuels; and other societal needs ( see my 2020 EPR lecture). Their achievement is blatantly prohibited by quantum mechanics due to its known time-reversal invariance compared to the strict irreversibility if the indicated processes. These basic societal needs, and their possible resolution via the Lie-admissible/Jordan- admissible"completion" of quantum mechanics into hadronic mechanics (see
Volume I: Mathematical Foundations, Volume II: Theoretical Foundations, and Volume III: experimental Verifications) were discussed at length during the 2020 International Teleconference on Einstein's Determinism, see the recorded lectures and comments http://www.world-lecture-series.org/level-xii-epr-teleconference-2020. The criticisms presented in Post 79 deal with isolated hadrons, nuclei and stars that can be assumed to be time-reversal invariant, thus requiring the Lie-isotopic/Jordan-isotopic branch of hadronic mechanics.
COUNTER-CRITICISM 1:
The "quantum nature of the observation" and Bell's inequality cannot be
formulated, let alone verified, for extended particles in deep mutual entanglement under non-linear, non-local and non-potential interactions (strong interactions).
COUNTER-CRITICISM 2: As clearly stated in Ref. [7], the realization T = Diag. (1/λ, λ) of the isotopic element T 'hidden' in the isoproduct ATB was introduced to honor the memory of David Bohm. As treated in detail in Tutoring Lecture I,
the isotopic element T represents "physical elements of reality" that cannot be treated via quantum mechanics, such as the size, shape, deformability, and density of hadrons as well as their non-linear, non-local and non-Hamiltonian interactions. Ref. [7] illustrated the physical meaning of the isotopic element by achieving the first known numerically exact representation of nuclear magnetic moments thanks to the deformability of nucleons. Section .2.8 of Ref.[11] achieved the first known representation of all characteristics of the deuteron, including its spin 1 in the true ground state, thanks to the representation of strong nuclear forces via the isotopic element T.
COUNTER-CRITICISM 3"
The physical meaning of T has been identified above.
COUNTER-CRITICISM 4: Refs. [7-11] have shown the progressive recovering of Einstein's determinism with the increase of the density of hadrons, nuclei and stars, to reach 'crystal type' conditions at the limit of gravitational collapse under which quantum uncertainties have no conceptual, mathematical or physical meaning.
COUNTER-CRITICISM 5: Ref. [8] indicated that Einstein determinism is fully achieved for particles in the interior if black or brown holes whose center of mass can be identified with full classical precision. In regard to the uncertainties of nuclear constituents, Criticism 5 refers to the use of "quantum" measurements, that is, measurements at a distance, under "strong," interactions requiring measurements at contact, for which quantum measurements cannot be formulated, let alone used. R. M. Santilli.
Post 81
I suggested in the past, and I suggest again that Wikipedia should quote in Santilli's 'Article' the 1998 paper ,
R. M. Santilli, Acta Applicandae Mathematicae Vol. 50, 177 (1998) proving the existence of classical counterparts for extended hadrons in deep
mutual entanglement thanks to the "completion" of quantum mechanics into
hadronic mechanics. The indication of the achievement in said paper of the fist known numerically exact representation of nuclear magnetic moments should also deserve a mention for credibility. Additionally, I suggest that Wikipedia should quote in the indicated 'Article'
the 2019 paper R. M. Santilli, Ratio Mathematica Volume 37, pages 5-23 (2019) proving, again thanks to hadronic mechanics, the progressive recovering of Einstein's determinism in the interior of hadrons, nuclei and stars, and its full recovering at the limit of gravitational collapse. I finally suggest the quotation of the recent
International Teleconference on Einstein's Determinism
and related recorded lectures organized by the R. M. Santilli Foundation
and the Family of Israel Foundation during which event the indicated papers were discussed in detail.
Post 82
I believe that the 'criticisms' of hadronic mechanics voiced by Post 79 are similar to the criticisms in the early 1990s of quantum mechanics based on Newtonian mechanics.
Post 83
Re post 81, why don't you edit the w'pedia article yourself and add the reference? W'pedia is 'the encyclopedia that anyone can edit'. [in theory you are not supposed to edit an article about yourself but you can try. There shouldn't really be a problem here]
Post 84
Thanks post 83. I will do as suggested and report here the outcome [I am not Santilli].
Post 85
Post 84, I am very curious to see whether you will succeed in changing an iota in Wikipedia's article on Prof. Santilli.
Post 86
Post 78, referring to points 2 and 5, it seems you are taking the quadratic Casimir invariant, then taking the square root of both sides? My concern is that, in Einstein's derivation (which point 2 uses to infer positive mass from positive energy), he did not consider negative masses explicitly. Thus we cannot use E=mc^2 without deriving it in the isodual space as well.
Post 87
Post 83, this is a courtesy note to indicate that I need a few days for submitting the editing suggested in post 81 in order to learn W'pedia html commands and consult with Ruggero as well as other experts for accuracy. Thanks. Poster 81
Post 87
Re post 81, why don't you edit the w'pedia article yourself and add the reference? W'pedia is 'the encyclopedia that anyone can edit'. [in theory you are not supposed to edit an article about yourself but you can try. There shouldn't really be a problem here].n
Post 88
Post 87. There is a misunderstanding. I will edit the 'article' and assume full responsibility of its content. However, it is in my style to consult with experts prior to venturing judgment on things so complex as the verification of the EPR argument. Is this against W'pedia rules?
Post 89
Dear Post 81, what is Einstein's determinism?
I think you mean the ever known classical determinism as you already said ... R. M. Santilli proving the existence of classical counterparts ... of the "completion" of the QM into the hadronic mechanics.
I would say ... thanks to hadronic mechanics Prof. R. M. Santilli has recovered the classical determinism ..., which is really a very surprising result.
Post 90
Thanks Post 89. Yes, Prof. Santilli's achievement is quite remarkable for which reason he was in the extremely short final list of the candidates for the 2020 Nobel Prize in Physics. Poster 81.
Post 91
I am a newcomer to this debate. I have been following it since I am interested in the foundations of physics, and consequently in the EPR argument and various other contributions as well. It is clear to me that Prof. Santilli and coworkers have a powerfully coherent position that ought to enhance our understanding. It is also clear to me that truth is one, and therefore if the Santilli theorems appear to be inconsistent with another theorem then one of three things must be the case:
1. We don't properly understand the theorems
2. One of the theorems is in fact unproven
3. Both of the theorems are unproven.
And of course, a proof is essential to being a theorem.
Now I wish to comment on POST 37 and the reply to it by Prof. Santilli (POST 38). Goedel's Incompleteness Theorem fatally undermined the search by Russell and Whitehead for completeness in the axioms of arithmetic (and therefore, by extension, the whole of mathematics). Prof. Santilli has said several times that he is a "formula man"?, and indeed the Editors (in POST 40) claim that he is not (implying that he should not be) interested i "statements [that cannot] be turned into equations". In my opinion it is not sufficient to hide behind such technical formalism. Goedel's Theorem establishes that the statement "this statement is undecidable? can be formulated as a well formed formula in Peano Arithmetic, and consequently is not meaningless in that system. The technical apparatus needed to establish this formalism is rather formidable, nevertheless it was established. This proved sufficient to demonstrate that a consistent and sufficiently rich axiomatic system (such as Peano arithmetic) cannot be complete, that is, there must exist theorems (true statements) in the system that cannot be proved in the terms of that system. Now, Prof. Santilli says that he carefully uses the term "final"? rather than "complete"to describe the theory of hadronic mechanics, nevertheless it seems clear to me that Goedel's Theorem assures us, as a basic property of rationality itself, that any axiomatic representation of reality must necessarily be incomplete. This is simply because any consistent axiomatic system (whether or not it is a representation of reality) must itself be incomplete, allowing truths to be formulated in terms of the system which have no proof in the terms of the system. It seems to me that this is no criticism of Prof. Santilli's basic argument; however, it would be better to recognise that all our formal representations of reality will turn out to have limitations.
Post 92
Could someone put a two- three line overview of what all this Einstein data is about . I know it is complicated but as a trained food technologist I have my limits and would be interested in a brief overview of its importance.
Post 93
Post 89, thank you. yes indeed Prof. Santilli is a favorite candidate. Could you please please answer my question on post 89, what do you mean with Einstein's determinism?
Post 94
Post 92, sorry for my late comments, but I thought the definition you use is correct. The only thing I can add is that, with his mathematical accuracy, Prof. Santilli does not use in his papers the words 'E instein's determinism,' and uses instead 'Einstein's isodeterminism' which means its definition and validity the way it was derived, that is, on isospaces over isofields. So colloquially, my view is that you can use your classical meaning of the words, but when dealing with calculations you have to use Santilli isomathematics.
Post 95
Post 91, to my understanding (note that I am not an expert), Goedel's theorem provides a strong support for Prof. Santilli's profs of Einstein's determinism. The sole issue I see in this debate is in the word "complete" used by Goedel which does not correspond to Einstein's "completion." For this reason, Prof. Santilli's uses Goedel's theorem with the word "final" instead of "complete." For instance, Prof. santilli "completed" quantum mechanics " into the Lie-admissible genomechanics for the representation of irreversible processes. Yet he stressed repeatedly that genomechanics should not be considered as being a "final" theory. And in fact, thanks to the participation by the famed Greek mathematician Prof. Thomas Vougiouklis, genomechanics was "completed" into hypermechanics via the transition from single-values operations (2 x 3 = 6) to hyperoperations (2 x 3 = 10^30 results) which "completion" is necessary to represent living organisms. But again hypermechanics should not be considered as being "final," because broader formulations may appear in due time. In summary, I do not see any real issue because Goedel's theorem is indeed valid, and everybody can use preferred words once they are accurately defined.
Post 96
Dear post 94.
It is not personal taste when we discuss science, so classical determinism is the common scientific formulation for determinism!
Indeed, using 'Einstein's isodeterminism' is less confusing! I must add that if Prof. Santilli used this notation, that is up to him.
In my view, we generally refer as much as possible to the meaning of the physical results in the common scientific language, specifically that it should be clear and less confusing for the general public, in fact we are scientists, aren't we?
Post 97
Full agreement Post 96.
Post 98
It was shown at the 2020 Teleconference on Einstein's Determinism that, in accordance with Einstein's criterium, quantum mechanics may be considered within geometrical interpretation as a complete theory, see the lecture by Prof. O. A. Olkhov http://www.world-lecture-series.org/olkhov-possibility-of-geometrical-interpretation-of-hidden-variables
Post 99
Dear Post 95, Let me please express my disagreement with you.
I think that is a real issue.
And thank you Post 91 for bringing this up.
Let us look to the progonal epr-paper. The authors ask the question:
Can Quantum-Mechanical Description of Physical Reality Be Considered Complete'?
and they concluded: we have thus shown that the wave function does not provide a complete description of the physical reality.
Also note, see the epr-paper, that the authors motivation was that "In quantum mechanics it is usually assumed that the wave function does contain a complete description of the physical reality of the system in the state to which it corresponds."
I guess the problem was and still is that the most of the scientists/physicists are not familiar with Goedel's theorem. One usually thought/think that a complete description of the reality is possible, (or a final theory is possible, see Posts 37, 838).
I think in the epr-paper no (no clear or explicit) difference was made between a completion of quantum mechanics in a theory that describes the physical reality (to recover the classical determinism) and a theory in the sense of a final theory.
Prof. Santilli stated clearly in Post 38 that he did not mean a complete description of the reality (a final theory in his own word). I found the response of Prof. Santilli in Post 38 is satisfactory.
Prof. Santillit uses the notation completion of quantum mechanics in the sense of an extension, i.e. a completion (think also about hidden variables and the Bohmian mechanics) to recover the classical determinism and he used the notation 'Einstein's isodeterminism' to stress the relation to the epr-paper.
However, because the notation refers to the epr-paper, a confusion can happen.
A problem rises when one misunderstands this (completion), in relation to epr-paper. Then, a complete description of the reality given in the epr-paper differs from the completion of the quantum mechanics thought by Prof. Santilli. In other words, the complete description of the reality in the epr-paper is not possible due to the Goedel's theorem, whereas the completion of the quantum mechanics done by Prof. Santilli recovers the classical determinism (under some extreme conditions).
The issue becomes more clear when we look to the answer of Q7 above '' Einstein's main point was the lack of completion of quantum mechanics, namely, quantum mechanics is not the final theory of the universe due to the possible existence of a generalization "completion" (in Einstein's words) of quantum mechanics into a theory recovering classical determinism under limit
conditions.`And, the completion of the quantum mechanics (e.g. the hadronic mechanics) is not
(and can not due to the Goedel's theorem) a final theory of the universe too.
Best regards.
Post 100
Poster 99, definitely you are an expert in the field while myself, as stated, I am not. Poster 91
Post 101
Dear Poster 99. Thank you. In my view you have stated this correctly. Now, Roger Penrose has demonstrated that "classical determinism" is actually logically inconsistent in his "Road to Reality" (2004) with a very elegant mathematical argument. Moreover, Parker & Jeynes last year (http://dx.doi.org/10.1038/s41598-019-46765-w) demonstrated that there exists an entropic "Principle of Least Exertion" which is isomorphic to the kinematic "Principle of Least Action" that has been known since the 17th century. This permits a whole range of radically different sorts of calculation as can be seen in the cited paper and in the followup paper on the stability of Buckminsterfullerene.
I expect that this new approach (from a completely different entropic point of view) will prove to have a bearing on the EPR problem, perhaps putting new life into Bohm's "hidden variable" proposal.
Post 102
Post 1o1, please outline the view by Sir Roger Penrose on hidden variables so that we can compare it with the corresponding view by Sir Ruggero (Roger) Santilli. Thanks.
Post 103
It appears that Pst 101 is the best illustration Sir Karl Popper's schism in physics.
Post 104
EDITORIAL NOTE FOR POSTERS ON GOEDEL'S THEOREM. Please note we consider close the debate on the "English translation" of German words used by Kurt Goedel in his theorem. The sole additional post we can accept is the identification of the original German words used by Goedel by a German speaking scholar and the "list" of their English translations. This debate deals with verifications and applications of Einstein's view that 'quantum mechanics is an incomplete theory.' Hence, we shall continue to use hereon the word 'complete' in the sense intended by Einstein. Please understand that we cannot possibly change words used by Einstein just because of debates on the English translation of German words. Thank you. The EPR Editorial Team.
Post 105
Allow me to express my congratulations to Roger Penrose for his fully deserved 2020 Nobel Prize in Physics,
and to report the pleasure and the honor of meeting him during his visit in the early 1970s at the Department of Physics of Boston University where I was then in the faculty. I remember the beauty, rigor and elegance of his mathematical presentations followed by pleasant conversations, for instance, on the Lie-admissible formulation of nonconservative systems in statistical mechanics which I did with Paul Roman. Sincerely, Ruggero Maria Santilli
Post 106
Wikipedia fellow in Post 89, you have been kidding me indeed, as done against many during the past twenty years under total impunity, but I heard rumors that Wikipedia may be added as Defendant to the lawsuit
https://www.washingtonpost.com/technology/2020/10/20/google-antitrust-doj-lawsuit/
filed by our Justice Department against Google.
Post 107
Dear Editors, I can not understand why my post did not appear!. Here it is again. n Post 105, I think the debate started with the EPR's objection to the incompleteness of quantum mechanics, as said in Post 99.
Post 108
EDITORIAL NOTE: Post 113 is a clear illustration of our reason to terminate that type of posting because of expected endless discussions on the meaning of "incompleteness" which is left undefined by post 113. Again, this debates deals with explicit realizations of the EPR historical argument that "quantum mechanics is not a complete theory." and, to avoid a huge confusion, we have to restrict posts to the word "lack of completeness" or 'incompleteness" as clearly defined by EPR. We plan to set up a separate debate in the field of Goedel's theorem, which is that of logic and epistemology and, then, yes you can have all the discussions you want on the meaning of words. Please understand. Thank you.
Post 109
Thank you Editorial for post 114. Allow me please the following post.
Dear Post 109. One should not forget that Einstein born and grow up in Germany and
his German language was the same of Goedel's German language.
Hence, they both used the word complete in the same sense.
In my view hadronic mechanics accomplished or completed
(is a completion of) the quantum theory. However, a completed theory is not a complete theory in the sense of a final theory, as thought by Einstein and Goedel.
Thus, a complete theory used by both Einstein and Goedel has the same meaning of a final theory. Whereas a completion of quantum mechanics done by Prof. Santiili means that the quantum mechanics is completed in
a more general theory, which encompasses or includes the quantum mechanics at the limit of a point particle (by Santilli isodifferential calculus).
Hence, hadronic mechanics and quantum mechanics together describe (but
there are still open questions) the microscopic world of subatomic
or Hadrons, atoms and molecules.
Hadronic mechanics thanks to Prof. Santilli is a great completion of quantum mechanics and we have now a comprehensive theory for microscopic world.
A final theory, i.e. a complete theory that describes the physical reality as thought by EPR is, to our today's knowledge, not possible. Fortunately, we have "a model-dependent reality'' in the spirit of Stephen Hawking, see Post 33.
This gives great hope that one day we will gain a deep understanding of physical reality by widen and refining our knowledge and theories.
Post 110
EDITORIAL NOI\TE: Thank you post 115.
Post 111
Prof. Santilli, can the isodual theory of antimatter be considered to be another "completion" of quantum mechanics in the EPR sense?
Post 112
Yes, post 111. I could not consider charge conjugation ψc(t, r) = - ψ†(t, r) to be "complete" because it characterizes antiparticles in the same Hilbert space of particles with a consequential positive rest energy by therefore preventing, in my view, a quantitative representation of matter-antimatter annihilation (Two positive masses cannot annihilate into light ). For this reason, I suggested the "completion" of charge conjugation into the isodual map (denoted with the upper index d) ψd(t, r) = - ψ†(- t†, - r†), which is an anti-Hermitean map not only of wavefunctions, but also of all characteristics of matter, thus including the characterization of antiparticles via negative energies as predicted by Dirac in 1928, which characterization does indeed allow a representation of matter-antimatter annihilation. To prevent the historical violation of causality for negative energies in our spacetime, I was forced to conjugate all other aspects of 20th century applied mathematics, and prove its compatibility with experimental data on electromagnetic interactions,
resulting in the isodual branch of hadronic mechanics http://www.i-b-r.org/Elements-Hadrfonic-Mechanics.htm. R. M. Santilli.
Post 113
WHAT IS THE ORIGIN OF OUR INCREASINGLY ALARMING ENVIRONMENTAL PROBLEMS?
Various posts have requested an outline for the general public of teleconference [1] on verifications [2] - [6] of Einstein-Podolsky-Rosen argument that "Quantum mechanics is not a complete theory" [7]. To state it in a nutshell, quantum mechanics has been unable to solve our increasing alarming environmental problems following one century of failed attempts, and billions of dollars of public funds, due to known structural insufficiencies. By contrast, Einstein's "completions" of quantum mechanics and chemistry into hadronic mechanics [8] and chemistry [9] have provided a resolution of said insufficiencies and provided serious possibilities for the solution of our environmental problems. The issue in a nutshell is: how long can the academic-governmental complex continue to ignore Einstein's legacy on the lack of universal character of quantum mechanics before causing a scientific obscurantism of historical proportions? Here are a few examples among many:
1. Recycling of nuclear waste.
Following the EPA prohibition for storage in the Jucca mountain in Nevada, highly radioactive nuclear wasted is nowadays stored by nuclear power plants. A question raised during the Teleconference [1] is: for how long should this situation be allowed to continue prior to reaching evident catastrophic conditions? The only credible recycling of nuclear waste is their stimulated decay capable of reducing thousands of years of mean life to minutes. This recycling is incompatible with quantum mechanics while being permitted by hadronic mechanics in a variety of ways, for instance, via irradiation with synthesized pseudoprotons [10] that, being negatively charged are attracted by nuclei, resulting in an excess of positive nuclear charges under which 'naturally unstable' nuclei disintegrate (for additional recycling mechanisms ignored since Al Gore run for the U. S. Presidency, see Ref. [11] and lecture [12]). Note that low energy pseudoprotons are also attracted by tumor cells by therefore allowing a localized tumor treatment much less invasive and more effective than the current invasive use of high energy proton irradiation and other treatments.
2. Controlled nuclear fusion. Following seventy five years of failed attempts, to qualify for his/her job, a nuclear physicist in academia or in a governmental funding agency must know and admit that quantum mechanics cannot consistently represent nuclear fusions because the former theory is reversible over time while the latter fusions are irreversible, by therefore requiring Einstein's "completion" into an irreversible covering theory (for a review, see Section 1.3 of Ref. [4] and lecture [12]). Hadronic mechanics has been built to be irreversible over time, and be reversible as a particular case, by therefore permitting experimentally verified nuclear fusions without harmful radiations under development at Hadronic Technologies Corporation [13] that are controllable with a variety of engineering means [14] [15]. Therefore, the important questions is: how long should the academic-governmental complex be allowed to continue the investment of billions of dollars of public funds in quantum mechanical nuclear fusions that are known to fail, in total oblivion of Einstein's legacy, without initiating joint funding of basically new nuclear fusions based on suitably "completed" theories?
3. Fossil fuel combustion. As it is well known, our increasingly alarming environmental problems are due to the incomplete combustion of fossil fuels, because contaminants such as carbon monoxide (CO) and hydrocarbons (HC) released in the exhaust are themselves combustible. After one century of contaminating our environment, to qualify for his/her job, a chemist in academia or in a governmental funding agency must know and admit that quantum chemistry cannot consistently represent any type of combustion, because said theory is reversible over time while all combustions are irreversible (for a review, see again Section 1.3 of Ref. [4] and lecture [12]). By contrast, Einstein's "completion" of quantum chemistry into the irreversible hadronic chemistry has permitted the conversion of fossil fuels into the magnegas fuel with full combustion [16] that I developed when I was Chief Scientist of Magnegas Corporation ]17]. Hadronic chemistry has also permitted the formulation of a basically new principle of combustion under development at Hadronic Technologies Corporation [13]. Note that
hadronic chemistry has permitted the industrial synthesis of a new species of Oxygen, called Magne-Oxygen (MO) [16], which is composed by clusters of conventional Oxygen O2, O2 × O, O2 × O2, ...
which are solely permitted by the new magnecular bond "×". MO is stable at ambient temperature and decomposes into ordinary Oxygen when absorbed by lungs while emitting virus killing UV light. Hence,
it appears advisable to test the use of MO in ventilators in lieu of conventional Oxygen because it would resolve known instability problems in the use of Ozone in ventilators, while sterilizing and Oxygenating the invested area.
In summary, the question to be answered by people is: What are the scientific and societal origins of our increasingly alarming environmental
problems? Ruggero Maria Santilli.
REFERENCES
[1] 2020 International Teleconference on Einstein's Determinism,
Announcement in English
http://eprdebates.org/epr-conference-2020.php
Recorded lectures
http://www.world-lecture-series.org/level-xii-epr-teleconference-2020
[2] R. M. Santilli, ``Isorepresentation of the Lie-isotopic SU(2) Algebra with Application to Nuclear Physics and Local Realism," Acta Applicandae Mathematicae Vol. 50, 177 (1998),
http://www.eprdebates.org/docs/epr-paper-i.pdf
[3] R. M. Santilli, ``Studies on the classical determinism predicted by A. Einstein, B. Podolsky and N. Rosen," Ratio Mathematica Volume 37, pages 5-23 (2019),
http://www.eprdebates.org/docs/epr-paper-ii.pdf
[4] R.M. Santilli, ``Studies on A. Einstein, B. Podolsky, and N. Rosen prediction that quantum mechanics is not a complete theory, I: Basic methods,"
Ratio Mathematica Volume 38, pp. 5-69, 2020,
http://eprdebates.org/docs/epr-review-i.pdf
[5] R.M. Santilli, ``Studies on A. Einstein, B. Podolsky, and N. Rosen prediction that quantum mechanics is not a complete theory, II: Apparent proof of the EPR argument,"
Ratio Mathematica Volume 38, pp. 71-138, 2020,
http://eprdebates.org/docs/epr-review-ii.pdf
[6] R.M. Santilli, ``Studies on A. Einstein, B. Podolsky, and N. Rosen prediction that quantum mechanics is not a complete theory," III: Illustrative examples and applications,"
Ratio Mathematica Volume 38, pp. 139-222, 2020,
http://eprdebates.org/docs/epr-review-iii.pdf
[7] A. Einstein, B. Podolsky , and N. Rosen, ``Can quantum-mechanical description of physical reality be considered complete?,'' Phys. Rev., vol.~47 , p. 777 (1935),
http://www.eprdebates.org/docs/epr-argument.pdf
[8] R. M. Santilli, Elements of Hadronic Mechanics, Volumes I, II, III (1995 on), Ukraine Academy of Sciences
http://www.i-b-r.org/Elements-Hadrfonic-Mechanics.htm
[9] R. M. Santilli, Foundations of Hadronic Chemistry, with Applications to New Clean Energies and Fuels, Kluwer Academic
Publishers (2001),
http://www.santilli-foundation.org/docs/Santilli-113.pdf
Russian translation by A. K. Aringazin,
http://i-b-r.org/docs/Santilli-Hadronic-Chemistry.pdf
[10] R. M. Santilli,
``Apparent Experimental Confirmation of Pseudoprotons and
their Application to New Clean Nuclear Energies,"
International Journal of Applied Physics and Mathematics
Vol. 9, p. 72-100 (2019),
www.santilli-foundation.org/docs/pseudoproton-verification-2018.pdf
[11] Recycling nuclear waste, website
www.nuclearwasterecycling.com
[12] R. M. Santilli, "Historical aspects of Einstein's view that "quantum mechanics is not a complete theory," Lecture at Teleconference [1],
www.world-lecture-series.org/santilli-historical-aspects-on-einsteins-view-that-quantum-mechanics-is-not-a-complete-theory
[13] Hadronic Technologies Corporation, website
www.hadronictechnologies.com
[14] I. B. Das Sarma, "Comparison of various nuclear fusion reactors," Lecture at Teleconference [1],
http://www.world-lecture-series.org/das-sarma-comparison-of-various-nuclear-fusion-reactors-icns
[15] S. Beghella Bartoli, "Significance of the EPR argument for a new controlled nuclear fusion without Coulomb barrier," Lecture at teleconference [1],
http://www.world-lecture-series.org/beghella-bartoli-significance-for-the-epr-argument-of-a-new-controlled-nuclear-fusion-without-coulomb-barrier
[16] R. M. Santilli, "The novel sustainable Hyper-Combustion with no contaminants in the exhaust," invited plenary lecture at the summit SIPS, Hainan Island, China, Nov. 6 to 10, 2016,
http://www.youtube.com/watch?v=eyS6HDO5xDc&feature=youtu.be
2016 Frey International
Sustainability Award
http://www.youtube.com/watch?v=djuo2xAWDT8
[17] Magnegas Corporation, website
https://magnegas.com
[18] R. M. Santilli, "The novel magnecular species of hydrogen and oxygen with increased specific weight and energy content," Intern. J. Hydrogen Energy Vol. 28, 177-196 (2003),
http://http://www.santilli-foundation.org/docs/Santilli-38.pdf
[19] Y. Yang, J. V. Kadeisvili, and S. Marton, "Experimental Confirmations of the New Chemical Species of Santilli MagneHydrogen,"
International Journal Hydrogen Energy Vol. 38, page 5002 (2013),
http://www.santilli-foundation.org/docs/MagneHydrogen-2012.pdf
================================
Figure 3. An illustration of the main quantum mechanical criticism of the EPR argument, the impossibility of determining with absolute accuracy the distance "d" between two protons due to Heisenberg's uncertainty principle.
