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Algebraic Structures as the Foundation of Quantum Theories: Generalizing the Number System Operator (NSO) Paradigm_enru

G L Dedenko, S P Klykov, A A Orlovsky

Published Jan 1, 2025• 0 citations
Publisher
DOI
10.13140/rg.2.2.36077.50404/51

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Algebraic Structures as the Foundation of Quantum Theories: Generalizing the Number System Operator (NSO) Paradigm_enru

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We propose a unified framework where algebraic structures, rather than geometry, serve as the foundation of quantum theory. We derive the Hilbert space, canonical operators, and the uncertainty principle from an underlying algebra. The Number System Operator (NSO) model emerges as a concrete realization, linking precision (k), numerical base (B), and measurable quantities. We prove the non-commutativity of NSO projectors, introducing a “digital noise” as a new, testable form of uncertainty. We analyze its scale relative to Planck units and demonstrate Lorentz covariance of the NSO procedure, ensuring compatibility with special relativity. A roadmap for experimental verification is provided, suggesting high-precision spectroscopy, atomic clocks, and gravitational-wave interferometers as potential tests. This framework transforms conceptual ideas into a computable and physically relevant theory, bridging foundational physics, computation, and measurable predictions.

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We propose a unified framework where algebraic structures, rather than geometry, serve as the foundation of quantum theory. We derive the Hilbert space, canonical operators, and the uncertainty principle from an underlying algebra. The Number System Operator (NSO) model emerges as a concrete realization, linking precision (k), numerical base (B), and measurable quantities. We prove the non-commutativity of NSO projectors, introducing a “digital noise” as a new, testable form of uncertainty. We analyze its scale relative to Planck units and demonstrate Lorentz covariance of the NSO procedure, ensuring compatibility with special relativity. A roadmap for experimental verification is provided, suggesting high-precision spectroscopy, atomic clocks, and gravitational-wave interferometers as potential tests. This framework transforms conceptual ideas into a computable and physically relevant theory, bridging foundational physics, computation, and measurable predictions.
This paper introduces a unified operational framework that bridges combinatorial mathematics and nonlinear quantum mechanics by systematically developing the theory of generalized, degenerate, and rrr -extended operator-valued Stirling numbers and Bell polynomials. Constructed within the framework of the Generalized Heisenberg Algebra GHAf\text{GHA}_fGHAf​ , where the standard commutation relation is modulated by an analytic function of the Hamiltonian f(H)f(H)f(H) , these novel algebraic objects capture the intrinsic nonlinearity of deformed quantum systems. By implementing operational methods and evaluating operator actions on coherent and number states, we establish explicit representations, structural recurrence relations, and robust generating functions. We demonstrate that in the special case of f(H)=H+1f(H) = H + 1f(H)=H+1 , our operator-valued formulations gracefully reduce to their classical combinatorial counterparts, successfully recovering foundational milestones such as Dobinski’s formula.
We describe the large applicability of the Nonequilibrium Statistical Operator Method (NSOM) for the study of dissipative dynamic systems far from equilibrium. It is shown that the NSOM can be encompassed by a unifying variational principle, which produces a large family of NSO that contains existing examples as particular cases. Further, we review the application of the NSOM for the construction of a nonlinear quantum theory of large scope, and for the generation of a response function theory, for far-from-equilibrium Hamiltonian systems. An accompanying non-equilibrium thermodynamic Green's function theory is briefly described. Also it is shown that the NSOM provides mechano-statistical foundations for phenomenological irreversible thermodynamics, and for the important question of stability of far-from-equilibrium steady states and the emergence of self-organized dissipative structures in condensed matter.