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EQ(vT): Entropic Quantum — Vectorized Time. The Entropic Origin of Temporal Direction in Quantum State Space

Michael Adis

Published Mar 9, 2026• 0 citations
Publisher

Abstract

This work introduces a geometric framework in which the direction of time is identified with the normalized entropy gradient on quantum state space equipped with the Bures metric. The configuration space Γ = {ρ ∈ B(H) : ρ ≥ 0, Tr(ρ) = 1} is taken as the fundamental arena of physics — not an auxiliary description overlaid on a pre-existing spacetime, but the space from which spacetime structure may emerge. The von Neumann entropy S(ρ) = −Tr(ρ log ρ) defines a smooth scalar field on (Γ, g^B), and the time vector field T(ρ) = ∇S(ρ)/|∇S(ρ)| is its unit gradient. Five geometric consequences follow from this identification: (1) T is irrotational, implying a natural causal ordering; (2) the constant-entropy hypersurfaces Σ_c foliate Γ, suggesting spatial structure as entropy level sets; (3) the metric deformation g̃_μν = g^B_μν − 2T_μT_ν produces Lorentzian signature, with the coefficient −2 uniquely fixed by the requirement that T be unit timelike; (4) S acts as a global time function on (Γ, g̃), establishing stable causality and strongly constraining the formation of closed timelike curves; (5) K_μν = ∇^B_μ T_ν is symmetric and generates the extrinsic curvature of the entropy surfaces. These structures provide the geometric foundation from which gravitational dynamics are developed in the companion paper EFT: Entropic Field Theory. Within this framework the Wheeler–DeWitt equation HΨ = 0 can be interpreted as the condition ∇S_universe = 0: a closed system evolving unitarily preserves all eigenvalues of ρ, and therefore possesses no entropy gradient and no intrinsic time direction. The tension field f(ρ) = |∇S(ρ)| = √(Var_ρ(log ρ)) vanishes at two fixed points: the order pole (pure states on ∂Γ) and the chaos pole (the maximally mixed state). Time therefore disappears at both extremes, while physical processes occur in the interior region where f > 0. EQ(vT) establishes the geometric framework; the companion theory EFT provides the dynamical field equations.

DOI
10.5281/zenodo.18928791

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This work introduces a geometric framework in which the direction of time is identified with the normalized entropy gradient on quantum state space equipped with the Bures metric. The configuration space Γ = {ρ ∈ B(H) : ρ ≥ 0, Tr(ρ) = 1} is taken as the fundamental arena of physics — not an auxiliary description overlaid on a pre-existing spacetime, but the space from which spacetime structure may emerge. The von Neumann entropy S(ρ) = −Tr(ρ log ρ) defines a smooth scalar field on (Γ, g^B), and the time vector field T(ρ) = ∇S(ρ)/|∇S(ρ)| is its unit gradient. Five geometric consequences follow from this identification: (1) T is irrotational, implying a natural causal ordering; (2) the constant-entropy hypersurfaces Σ_c foliate Γ, suggesting spatial structure as entropy level sets; (3) the metric deformation g̃_μν = g^B_μν − 2T_μT_ν produces Lorentzian signature, with the coefficient −2 uniquely fixed by the requirement that T be unit timelike; (4) S acts as a global time function on (Γ, g̃), establishing stable causality and strongly constraining the formation of closed timelike curves; (5) K_μν = ∇^B_μ T_ν is symmetric and generates the extrinsic curvature of the entropy surfaces. These structures provide the geometric foundation from which gravitational dynamics are developed in the companion paper EFT: Entropic Field Theory. Within this framework the Wheeler–DeWitt equation HΨ = 0 can be interpreted as the condition ∇S_universe = 0: a closed system evolving unitarily preserves all eigenvalues of ρ, and therefore possesses no entropy gradient and no intrinsic time direction. The tension field f(ρ) = |∇S(ρ)| = √(Var_ρ(log ρ)) vanishes at two fixed points: the order pole (pure states on ∂Γ) and the chaos pole (the maximally mixed state). Time therefore disappears at both extremes, while physical processes occur in the interior region where f > 0. EQ(vT) establishes the geometric framework; the companion theory EFT provides the dynamical field equations.
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This paper introduces the Total Entropic Quantity (TEQ) framework, a structural reformulation of quantum theory grounded in two foundational axioms. Axiom 0 posits entropy as a generative constraint: a geometric principle that determines which configurations can stably distinguish themselves, independent of space, time, or dynamics. Here, entropy is defined as a curvature-functional over distinguishability configurations, preserving only those patterns that remain stable under finite informational resolution---that is, structures not dissolved by coarse-graining or limited observability. Axiom 1, the Minimal Principle (MP), selects from these structures those that are maximally stable under entropy-weighted variation. From this entropic foundation, core elements of quantum theory---including the Born rule, quantization, and Schrödinger dynamics---emerge as special cases of entropy-stabilized geometry. The framework derives an entropy-weighted path integral and introduces a corrected Schrödinger equation that governs evolution in regimes of finite entropy curvature. In the high-resolution limit (β→∞ \beta \to \infty β→∞), TEQ reduces to standard unitary quantum mechanics; in more general regimes, entropy flow deforms canonical dynamics, linking decoherence, dissipation, and gravitational curvature. TEQ reinterprets physical law as emergent structure within the geometry of distinguishability, rather than as imposed dynamics on a fixed spacetime background.
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This paper introduces the Total Entropic Quantity (TEQ) framework, a structural reformulation of quantum theory grounded in two foundational axioms. Axiom 0 posits entropy as a generative constraint: a geometric principle that determines which configurations can stably distinguish themselves, independent of space, time, or dynamics. Here, entropy refers to a curvature-functional over distinguishability configurations, maintaining only those structural patterns that remain stable or well-posed under finite informational resolution—that is, structures that are not destroyed or dissolved by coarse-graining or limited observability. Axiom 1, the Minimal Principle (MP), selects from these configurations those that remain maximally resolvable under finite entropy resolution. From this entropic foundation, core features of quantum theory—including the Born rule, Schrödinger dynamics, quantization, and gravitational structure—emerge as consequences of variation within an entropy-curved geometry. TEQ unifies quantum coherence, classical emergence, and spacetime curvature under a single informational principle, replacing conventional postulates with entropy-stabilized structure. The framework predicts deviations in high-curvature regimes and reinterprets physical law as the geometry of distinguishability rather than imposed dynamics.
Entanglement for pure bipartite states is most commonly quantified in a state-by-state manner to each pure state of a bipartite system a scalar quantity, such as the von Neumann entropy of a reduced density matrix. This provides a precise local characterization of how entangled a given state is. At the same time, this local description naturally invites a set of complementary, more global questions about the structure of the space of pure states: How abundant are the states with a given amount of entanglement within the full state space? Do the manifolds of constant entanglement exhibit distinct geometric regimes? These questions shift the focus from assigning an entanglement value to a single state to understanding the global organization and geometry of entanglement across the entire manifold of pure states. In this work, we develop a geometric framework in which these questions become natural. We regard the projective Hilbert space of pure states, endowed with the Fubini-Study metric, as a Riemannian manifold and promote bipartite entanglement to a macroscopic functional on this manifold. Its level sets stratify the space of pure states into hypersurfaces of constant entanglement, and we define a geometric entanglement entropy as the log-volume of these hypersurfaces, weighted by the Fubini-Study gradient of entanglement. This quantity plays the role of a microcanonical entropy in entanglement space: it measures the degeneracy of a given entanglement value in the natural quantum geometry. The framework is illustrated first in the simplest case of a single spin-1/2 and then for bipartite entanglement of spin systems, including a two-qubit example where explicit calculations can be carried out, along with a sketch of the extension to spin chains.