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arXiv:physics/0512018

Chiral quantum mechanics (CQM) for antihydrogen systems

Guido van Hooydonk

Published Dec 3, 2005• 0 citations
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Abstract

A first deception of QM on antiH already appears in one-center integrals for two-center systems (G. Van Hooydonk, physics/0511115). In reality, full QM is a theory for chiral systems but the QM establishment was wrong footed with a permutation of reference frames. With chiral quantum mechanics (CQM), the theoretical ban on natural antiH must be lifted as soon as possible.

DOI
10.48550/arxiv.physics/0512018

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•Aug 1, 2025•1 citation
A first deception of QM on antiH already appears in one-center integrals for two-center systems (G. Van Hooydonk, physics/0511115). In reality, full QM is a theory for chiral systems but the QM establishment was wrong footed with a permutation of reference frames. With chiral quantum mechanics (CQM), the theoretical ban on natural antiH must be lifted as soon as possible.
The internal microscopic phase transition in atom H described with a Hund-type Mexican hat potential is analytically congruent with the macroscopic phase transitions between states of aggregation, described with classical Van der waals-Maxwell binodals and spinodals. This means the UEOS (universal equation of state) exists and is valid for any phase transition in any system. A universal chiral symmetry breaking mechanism applies to BEC, where the de Broglie length is important. We show quantitatively that his standing wave equation leads to the equivalence of macro- and microscopic phase transitions, due to natural chiral symmetry breaking. The experimentally detected phase transition in the so-called simple Coulomb electron-proton bond between the 2 enantiomers H and antiH is the generic prototype.
We extend our proof of mathematical equivalence between quantum and classical mechanics to interacting systems, towards the the complete unification framework. By demonstrating that reference frame integration of classical interacting trajectories yields the exact quantum propagators for multi-particle systems, we show that quantum entanglement emerges naturally from correlated reference frame transformations of classical dynamics. The key insight is that reference frame democracy and interaction dynamics operate on orthogonal degrees of freedom: boosts affect only center-of-mass motion while interactions govern relative coordinates. This factorization explains why quantum mechanics naturally separates into free center-of-mass propagation and interacting relative motion. We provide explicit derivations for two-particle systems with arbitrary interactions V(r), demonstrate the emergence of quantum bound states from classical orbital motion, and prove that the entire mathematical apparatus of non-relativistic quantum mechanics is equivalent to classical mechanics for interacting systems, viewed through the lens of reference frame democracy. The pencil dot insight thus extends further its revolutionary implications: there is no separate quantum world---only classical reality properly accounting for Einstein's relativity.