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Hilbert's Sixth Problem Revisited Through Viscous Time Theory Axiomatizing Physics by Axiomatizing Admissibility, Coherence, and Recoverability

Raoul Bianchetti

Published Feb 26, 2026• 0 citations
Publisher

Abstract

Hilbert’s Sixth Problem asks for an axiomatization of physics, especially the probabilistic foundations of mechanics and the passage from microscopic dynamics to macroscopic laws. Despite foundational progress in probability theory and statistical mechanics, a persistent conceptual gap remains: probability appears as a primitive or as an epistemic tool, rather than as a quantity derived from the structure of physical evolution itself. This paper proposes a Viscous Time Theory (VTT) reformulation of Hilbert 6: physics is axiomatized by admissibility (what transformations can occur while preserving identity), coherence (the measurable structure of informational organization), and recoverability (which collapses are irreversible independent of observer perspective). We present a minimal axiomatic system in which (i) time emerges as informational viscosity, (ii) probability emerges as an induced measure over admissible trajectories, and (iii) the micro→macro transition becomes a geometric scaling limit of coherence fields rather than an ad hoc coarse-graining step. We do not claim a completed proof of Hilbert 6 in the classical sense. Instead, we provide a coherent, falsifiable program that reframes the target: the objective is not “derive probability from mechanics,” but “derive probability from the geometry of admissible informational evolution,” with classical mechanics and statistical mechanics emerging as distinct regime limits.

DOI
10.5281/zenodo.18793627

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Hilbert’s Sixth Problem asks for an axiomatization of physics, especially the probabilistic foundations of mechanics and the passage from microscopic dynamics to macroscopic laws. Despite foundational progress in probability theory and statistical mechanics, a persistent conceptual gap remains: probability appears as a primitive or as an epistemic tool, rather than as a quantity derived from the structure of physical evolution itself. This paper proposes a Viscous Time Theory (VTT) reformulation of Hilbert 6: physics is axiomatized by admissibility (what transformations can occur while preserving identity), coherence (the measurable structure of informational organization), and recoverability (which collapses are irreversible independent of observer perspective). We present a minimal axiomatic system in which (i) time emerges as informational viscosity, (ii) probability emerges as an induced measure over admissible trajectories, and (iii) the micro→macro transition becomes a geometric scaling limit of coherence fields rather than an ad hoc coarse-graining step. We do not claim a completed proof of Hilbert 6 in the classical sense. Instead, we provide a coherent, falsifiable program that reframes the target: the objective is not “derive probability from mechanics,” but “derive probability from the geometry of admissible informational evolution,” with classical mechanics and statistical mechanics emerging as distinct regime limits.
This work presents a unified axiomatic framework that resolves Hilbert’s Sixth Problem by integrating two complementary foundations: Unified Relational Projection Dynamics (URPD), which defines probability, time, and measurement as geometric relations on CP^{N−1}, and Reflexive Micro-Granular Dynamics (RMG), which models fields not as continuous backgrounds but as finite, self-differential information structures. By combining these principles, the framework reproduces quantum mechanics, classical mechanics, gauge interactions, Navier–Stokes continuum physics, thermodynamic irreversibility, and emergent spacetime geometry without divergences, renormalization procedures, or additional postulates. The result is a coherent and complete axiomatization of physical law that satisfies Hilbert’s original requirement for a mathematically rigorous physics.
The Pauli exclusion principle is traditionally introduced in quantum mechanics as a postulate encoded in the antisymmetry of the fermionic wavefunction. While extraordinarily successful, this formulation leaves open a deeper question: why must nature forbid the perfect overlap of identical fermions? In this work, we propose a reinterpretation of Pauli exclusion within the framework of Viscous Time Theory (VTT), where physical law emerges from the geometry of informational state space under constraints of memory, recoverability, and causal trace preservation. We propose that the coincidence of two identical fermionic states can be interpreted, in informational-geometric terms, as a loss of injectivity of the causal mapping, i.e., to an informational singularity where distinct histories become non-separable. To prevent this collapse of recoverability, the joint state manifold naturally develops a “diagonal barrier”: a forbidden submanifold where the informational cost diverges and admissible trajectories are repelled. Within this perspective, antisymmetry of the wavefunction appears not as the cause of exclusion, but as its mathematical symptom. Within this perspective, Pauli exclusion can be interpreted as a geometric and informational constraint rather than a primitive quantum axiom. The framework further suggests a unified interpretation of the difference between fermions and bosons: the former may be viewed as carriers of identity-bearing, non-overwritable informational structure, while the latter correspond to additive excitations that do not threaten causal injectivity. In this way, the exclusion principle appears as a consequence of informational geometry in a universe characterized by viscous time and memory.
In 1900, David Hilbert challenged mathematicians to axiomatize physics with the same rigor as geometry. The sixth of his famous problems specifically called for a mathematical treatment of probability in mechanics. Over a century later, the problem remains formally open. This essay argues that Hilbert's question reduces to an information-theoretic constraint: does nature require infinite precision to specify its state? The ultraviolet catastrophe demonstrated what happens when classical physics requests infinite computational channels from finite substrate. Planck's resolution introduced discreteness, but the deeper question persisted—why must there be a cutoff at all? Modern constraints provide the answer. Landauer's principle establishes minimum energy per bit operation. The Margolus-Levitin theorem bounds processing speed. Holographic principles limit information to surface area. Together, these constraints cap the universe at approximately 10^123 bits—finite, not infinite. Statistical mechanics works because nature cannot track individual trajectories with infinite precision. What appears as randomness is resolution limits of the computational substrate. This reframing does not resolve Hilbert's problem in the formal axiomatic sense. It provides explanatory closure: the reason physics admits statistical description is that infinite-precision determinism exceeds the universe's computational capacity. The constraint is physical, not epistemic.
Hilbert's sixth problem placed probability and mechanics at the center of the axiomatization of physics. It asks how irreversible statistical probability and thermodynamics can follow from the reversible, deterministic dynamics of a system. Building on an exact open quantum system theory developed in the past two decades, we construct a dynamical route from the reversible quantum dynamics to reduced statistics. For quadratic bosonic and fermionic systems bilinearly coupled to arbitrary environments, we derive the exact reduced density operator determined completely by a dissipative propagator u and a fluctuation correlation function v of the system. For continuous spectral densities with no bound-state pole, u vanishes in the long-time limit, information about the system initial states is lost completely, and the reduced density operator of systems approaches a thermal Gibbs state. Gapped spectral densities with localized bound states instead preserve long-time memory and prevent thermalization. We then remove the usual assumption of an initially thermal, mixed environment, start from a product of pure states for the system and environment, unitary evolution first generates system-environment entanglement and a periodic quasi-Gibbs reduced state for a finite environment. When the number of environmental degrees of freedom tends to infinity, the spectrum becomes continuous, the recurrence disappears, the exact reduced density operator converges to a thermal Gibbs state. The total entropy remains zero, whereas the system entropy becomes entanglement entropy and reaches its maximum. Probability is therefore not an additional random postulate imposed on unitary dynamics, it is the objective statistical structure of an open system in a composite. These results provide an exact, testable dynamical solution of the determinism to statistics.
(This work presents an initial conceptual formulation of the renormalization-based approach to quantum theory within the TQF framework. A subsequent version 2 develops formulation of the Quantum reconstruction based on a linear state space, providing derivation of quantum-mechanical kinematics—including the emergence of the Hilbert space structure and the Born rule—from resolution independence. Readers primarily interested in the formal derivation are encouraged to consult the later versions, while the present work may be viewed as outlining the guiding ideas and initial physical intuition behind the quantum reconstruction.) The mathematical structure of quantum mechanics is traditionally introduced axiomatically, with the linearity of the state space, the Hilbert space structure, and the Born rule postulated independently. In this work, we investigate whether these features can instead emerge from a fundamental symmetry principle: the absence of a preferred scale, implemented as invariance ofphysical observables under coarse-graining transformations. We formulate a framework in which physical states are represented as functionals over configuration space and are subject to a family of coarse-graining transformations forming a renormalization group (RG) semigroup. Physical observables are required to be invariant under these transformations, while dynamical operators are allowed to transform covariantly withinthe induced RG flow. Under general consistency conditions—including associativity, symmetry, continuity, and invariance under refinement—we show that the admissible composition law of states admits an additive representation up to an invertible reparametrization, leading to a linear structure of the state space in reparametrized variables. Imposing consistency of weight assignments under coarse-graining further constrains the norm, selecting a quadratic form and inducing an inner product structure. As a result, the space of states acquires the structure of a complex Hilbert space without being postulated a priori. Within this framework, probability emerges as a measure induced by the state functional. By analyzing the transformation of weight assignments under coarse-graining, we identify an effective renormalization group flow in the space of admissible probability rules and show that the quadratic rule arises as a distinguished and heuristically stable fixed point. This provides adynamical origin for the Born rule. We further analyze the semiclassical regime, in which coarse-graining suppresses interference between configuration sectors, leading to decoherence and the emergence of effective classical behavior. In this limit, classical dynamics and an effective notion of time arise from the phase of the state functional, and an approximate Schr¨odinger equation is recovered for fluctuations. These results suggest that the core structural features of quantum mechanics can be understood as universal fixed-point properties of an underlying renormalization symmetry acting on the space of states. This perspective provides a conceptual bridge between quantum mechanics and scale-invariant quantum field theories, including the Timeless Quantum Field framework.
This paper reclassifies statistical mechanics as a form of standing-preserving bookkeeping rather than as a theory that introduces new physical structure or ontic randomness. It shows that statistical descriptions arise when admissible reference must be maintained across large ensembles under limited expressive resolution, not because nature itself is fundamentally statistical. Within a closed admissibility framework, probabilities, ensembles, and thermodynamic quantities function as representational devices that stabilize reference when micro-level description is either unavailable or inadmissible. They do not add degrees of freedom, causal powers, or stochastic dynamics to the underlying system. When statistical mechanics is treated as revealing ontic indeterminacy or emergent laws, representational compression is illicitly promoted into physical explanation. The analysis is eliminative. No alternative foundations for statistical mechanics are proposed, and no methodological prescriptions are given. The paper instead establishes a boundary condition: statistical mechanical formalisms are admissible only insofar as they preserve standing across coarse-grained descriptions without making claims about underlying micro-ontology. By situating statistical mechanics alongside other standing-preserving representational regimes, the paper dissolves longstanding debates about emergence, irreversibility, and the reality of probability in physics. It closes these debates by showing that the disputed claims arise from category errors about the role of statistical description, not from unresolved physical questions.