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HADRONIC MATHEMATICS, MECHANICS AND CHEMISTRY 33
experts, to qualify as such, know that the representation requires a structural
modification of the basic axiom of expectation values as well as for numerous
additional reasons, such as:
1) The Bose-Einstein correlation is necessarily due to contact, nonpotential,
nonlocal-integral effects originating in the deep overlapping of the hyperdense
charge distributions of protons and antiprotons inside the fireball;
2) The mathematical foundations of quantum mechanics (such as its topology),
let alone its physical laws, are inapplicable for a meaningful representation of said
nonlocal and nonpotential interactions as outlined in preceding sections; and
3) Special relativity is also inapplicable, e.g., because of the inapplicability of
the basic Lorentz and Poincaré symmetries due to lack of a Keplerian structure,
the approximate validity of said theories remaining beyond scientific doubt.
Admittedly, there exist a number of semiphenomenological models in the literature
capable of a good agreement with the experimental data. Scientific deception
occurs when these models are used to claim the exact validity of quantum
mechanics and special relativity since the representation of experimental data
requires necessary structural departures from basic quantum axioms.
Of course, the selection of the appropriate generalization of quantum mechanics
and special relativity for an exact representation of the Bose-Einstein correlation
is open to scientific debate. Scientific deception occurs when the need for such a
generalization is denied for personal gains.
As we shall see, relativistic hadronic mechanics provides an exact and invariant
representation of the experimental data of the Bose-Einstein correlation at
high and low energies via unadulterated basic axioms, by providing in particular
a direct representation of the shape of the p − ¯p fireball and its density,
while recovering the basic invariant under a broader realization of the Poincaré
symmetry.
An in depth investigation of all applications of quantum mechanics and special
relativity at large reveals that they have provided an exact andinvariant representation
from unadulterated basic axioms of all experimental data of the hydrogen
atom, as well as of physical conditions in which the mutual distances of particles
is much bigger than the size of the charge distribution (for hadrons) or of the
wavepackets of particles (for the case of the electron).
1.2.10 The Scientific Imbalance in Nuclear Physics
There is no doubt that quantum mechanics and special relativity permitted historical
advances in also nuclear physics during the 20-th century, as illustrated, for
instance, by nuclear power plants. However, any claim that quantum mechanics
and special relativity are exactly valid in nuclear physics is a scientific deception,
particularly when proffered by experts, because of the well known inability of
these theories to achieve an exact and invariant representation of numerous nu-