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Journal of Physics: Applications and Mechanics

The Universal Refined Equation (CUP-Ω*): Covariant GKLS Dynamics, Tomonaga–Schwinger Integrability, and Einstein Langevin Coupling in the CUCE/ Spinoza/Hilbert Framework

Review Article | Open Access | Volume 13 | Issue 1
Article DOI :

  • 1. Campo Unificado de la Consciencia–Existencia (CUCE), Finis Terrae University, Chile
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Corresponding Authors
Vicente Merino Gallardo, Campo Unificado de la Consciencia–Existencia (CUCE), Finis Terrae University, Chile.
Abstract

We present a covariant, completely positive and thermodynamically consistent refinement of the universal equation within the CUCE/Spinoza/Hilbert framework, denoted CUP-?*. The formulation unifies Tomonaga–Schwinger evolution on Cauchy hypersurfaces with a modular Gorini–Kossakowski–Lindblad Sudarshan (GKLS) generator that obeys detailed balance in the GNS metric with respect to a unified thermodynamic target σ*. We prove (i) foliation independence under local commutation, (ii) complete positivity of the finite-step propagator, (iii) existence of a global Lyapunov functional https://www.jscimedcentral.com/public/assets/images/uploads/image-1770783030-1.JPG DS ensuring the second law, (iv) primitivity with a unique attractor σ*, and (v) local conservation via consistent coupling to the Einstein–Langevin equation with conserved stochastic sources. We further outline falsifiable predictions with quantitative protocols in superconducting circuits and optomechanics.

Keywords

• Covariant Open Quantum Systems; Quantum Markov Semigroups; Detailed Balance; Tomonaga Schwinger Equation; Stochastic Gravity; Information Geometry; Thermodynamic Learning 1

Citation

Gallardo VM (2026) The Universal Refined Equation (CUP-?*): Covariant GKLS Dynamics, Tomonaga–Schwinger Integrability, and Ein stein–Langevin Coupling in the CUCE/Spinoza/Hilbert Framework. J Phys Appl and Mech 3(1): 1016.

INTRODUCTION

Spinoza’s monism can be operationally reformulated in Hilbert-space language: one substance, many modes as observable algebras. Within this CUCE/Spinoza/Hilbert programme, the CUP-?∗ equation supplies a universal dynamical law that is (a) covariant at the level of foliation by Cauchy hypersurfaces, (b) completely positive at finite steps, and (c) thermodynamically consistent via a modular target https://www.jscimedcentral.com/public/assets/images/uploads/image-1770783232-1.JPGcapturing both KMS equilibrium and observer/prior information through an affine geometric mean. Our presentation emphasizes rigorous mathematical structure and empirical consequences.

MAIN EQUATION

Let ρ[Σ] be the state functional on a Cauchy hypersurface Σ. The local Tomonaga–Schwinger (TS) evolution at x ∈ Σ reads

https://www.jscimedcentral.com/public/assets/images/uploads/image-1770783297-1.JPG

The jump operators are modular with respect to the unified thermodynamic target https://www.jscimedcentral.com/public/assets/images/uploads/image-1770783357-1.JPG

https://www.jscimedcentral.com/public/assets/images/uploads/image-1770783411-1.JPG

https://www.jscimedcentral.com/public/assets/images/uploads/image-1770783458-1.JPG

Where denotes the affine geometric mean. Equation (1) couples to semiclassical gravity via a conserved stochastic source through 

https://www.jscimedcentral.com/public/assets/images/uploads/image-1770783510-1.JPG

Axioms

(Causal) Local commutation. For spacelike separated x, y, the local superoperators commute: https://www.jscimedcentral.com/public/assets/images/uploads/image-1770783592-1.JPG and https://www.jscimedcentral.com/public/assets/images/uploads/image-1770783639-1.JPG (CPTP) Bochner positivity. https://www.jscimedcentral.com/public/assets/images/uploads/image-1770783695-1.JPG and the rates https://www.jscimedcentral.com/public/assets/images/uploads/image-1770783740-1.JPG arise from positive-definite (Bochner) environment correlators so that https://www.jscimedcentral.com/public/assets/images/uploads/image-1770783799-1.JPG (GNS) Detailed balance. With modular jumps (2), the generator is symmetric in the GNS inner product https://www.jscimedcentral.com/public/assets/images/uploads/image-1770783872-1.JPG (Prim) Primitivity. The set https://www.jscimedcentral.com/public/assets/images/uploads/image-1770783938-1.JPG generates the full local ∗-algebra https://www.jscimedcentral.com/public/assets/images/uploads/image-1770783993-1.JPG in the spectral basis of https://www.jscimedcentral.com/public/assets/images/uploads/image-1770784048-1.JPG implying a unique faithful stationary state. 

(Cons) Conservation and gauge. are BRST-invariant; (4) uses conserved noise with fluctuation–dissipation relations.

Global Lyapunov functional and the second law

https://www.jscimedcentral.com/public/assets/images/uploads/image-1770784141-1.JPG

Theorem 1 (Monotonicity and exponential convergence). Under axioms (GNS) and (CPTP), https://www.jscimedcentral.com/public/assets/images/uploads/image-1770784196-1.JPG If in addition (Prim) holds, then https://www.jscimedcentral.com/public/assets/images/uploads/image-1770784254-1.JPG exponentially with a rate bounded below by the GNS spectral gap https://www.jscimedcentral.com/public/assets/images/uploads/image-1770784313-1.JPG Proof. Modularity (2) implies GNS symmetry [1]: https://www.jscimedcentral.com/public/assets/images/uploads/image-1770784357-1.JPG Hence https://www.jscimedcentral.com/public/assets/images/uploads/image-1770784412-1.JPG  is positive in this metric and coincides with the gradient of https://www.jscimedcentral.com/public/assets/images/uploads/image-1770784454-1.JPG yielding monotonicity. Primitivity makes the zero eigenspace one-dimensional and opens a spectral gap; the GNS Poincaré inequality then gives exponential decay of Φ.

Finite-step complete positivity

Theorem 2 (Finite-step CPTP). https://www.jscimedcentral.com/public/assets/images/uploads/image-1770784537-1.JPG come from positive-definite correlators (Bochner), the finite-step propagator https://www.jscimedcentral.com/public/assets/images/uploads/image-1770784584-1.JPG Proof. The GKLS form ensures complete positivity of infinitesimal maps with Kossakowski matrix positive semidefinite [2,3]. The kernel https://www.jscimedcentral.com/public/assets/images/uploads/image-1770784642-1.JPG makes the finite-step map a convex average of CP maps. Trace preservation follows from the Lindblad form. 

Primitivity and uniqueness of the attractor

Theorem 3 (Unique fixed point). If https://www.jscimedcentral.com/public/assets/images/uploads/image-1770784715-1.JPG generates the full local algebra, the semigroup is primitive: ker https://www.jscimedcentral.com/public/assets/images/uploads/image-1770784758-1.JPG and the stationary state is unique. Proof. Irreducibility implies that the commutant of https://www.jscimedcentral.com/public/assets/images/uploads/image-1770784878-1.JPG andard quantum semigroup theory then yields uniqueness of the fixed point and a positive spectral gap. 

TS integrability and causality

Theorem 4 (Foliation independence). If https://www.jscimedcentral.com/public/assets/images/uploads/image-1770784990-1.JPG and https://www.jscimedcentral.com/public/assets/images/uploads/image-1770785039-1.JPG Satisfies the hypersurface deformation algebra, then the TS evolution is independent of the chosen foliation Σ.

Proof. Adapt Schwinger’s argument: local commutators integrate to zero over spacelike-separated elements, ensuring path-independence of the ordered exponential along deformations of Σ. 

Conservation and Einstein–Langevin coupling

Theorem 5 (Local conservation). With conserved noise https://www.jscimedcentral.com/public/assets/images/uploads/image-1770785141-1.JPG and fluctuation–dissipation relations, and including the Lamb-shift https://www.jscimedcentral.com/public/assets/images/uploads/image-1770785204-1.JPG the renormalized stress tensor satisfies https://www.jscimedcentral.com/public/assets/images/uploads/image-1770785256-1.JPG and (4) is consistent with Bianchi identities.

Falsifiability and quantitative predictions

We outline protocols that access the modular structure and the conserved stochastic back-reaction:

1. Entropy production bound in a qubit. Engineering {Fa} to be the full set of matrix units on a superconducting qubit makes the dynamics primitive. The relative-entropy half-life obeys https://www.jscimedcentral.com/public/assets/images/uploads/image-1770785343-1.JPG we predict https://www.jscimedcentral.com/public/assets/images/uploads/image-1770785388-1.JPG .

2. For Equilibrium test of the unified target. For a 5 GHz qubit at T = 50 mK, the KMS factor is https://www.jscimedcentral.com/public/assets/images/uploads/image-1770785443-1.JPG and the excited-state fraction is https://www.jscimedcentral.com/public/assets/images/uploads/image-1770785498-1.JPG Any deviation explained by https://www.jscimedcentral.com/public/assets/images/uploads/image-1770785548-1.JPG in (3) can be estimated by tomography.

3. Choi test of finite-step CPTP. Reconstruct the Choi matrix of the propagator over a finite TS “slab”; positivity must hold within uncertainties fixed by the noise kernel.

4. Optomechanical probe of conserved noise. For a membrane of mass https://www.jscimedcentral.com/public/assets/images/uploads/image-1770785627-1.JPG the on-resonance displacement noise floor is https://www.jscimedcentral.com/public/assets/images/uploads/image-1770785691-1.JPG at room temperature; a conserved Einstein–Langevin contribution at the level of https://www.jscimedcentral.com/public/assets/images/uploads/image-1770785766-1.JPG of thermal noise would be marginally resolvable with state-of-the-art interferometry.

Limiting regimes

The principal asymptotic limits of CUP-?∗ and the corresponding recovered theories are summa- rized in Table 1. 

Figures (TikZ/PGFPlots)

METHODS

GNS detailed balance and modular jumps. Choosing https://www.jscimedcentral.com/public/assets/images/uploads/image-1770785989-1.JPG self-adjoint in the GNS inner product and pins https://www.jscimedcentral.com/public/assets/images/uploads/image-1770786042-1.JPG as the unique fixed point under (Prim). This identifies the flow with a gradient flow for https://www.jscimedcentral.com/public/assets/images/uploads/image-1770786085-1.JPG in the sense of quantum information geometry [1] (Figure 1).

https://www.jscimedcentral.com/public/assets/images/uploads/image-1770786148-1.JPG

Figure 1 Local TS block: unitary plus modular GKLS applied on a surface element.

Finite-step CPTP with Bochner kernels. Bochner positivity guarantees the Kossakowski matrix is positive semidefinite; the finite-step propagator is a convex mixture of infinitesimal CPTP maps, hence CPTP (Figure 2).

https://www.jscimedcentral.com/public/assets/images/uploads/image-1770786221-1.JPG

Figure 2 Local integrability under spacelike separation..

Einstein–Langevin consistency. Conserved noise ensures https://www.jscimedcentral.com/public/assets/images/uploads/image-1770786272-1.JPG Bianchi identities then ensure compatibility of (4) (Figure 3). 

https://www.jscimedcentral.com/public/assets/images/uploads/image-1770786331-1.JPG

Figure 3 Typical Lyapunov descent of relative entropy with rate bound 2λgap.

Data availability: No datasets were generated or analysed for this theoretical study.

Code Availability: All LaTeX/TikZ/PGFPlots code to reproduce the manuscript is included in the accompanying project.

Author Contributions: VMG conceived the CUP-?∗ framework, developed the mathematical proofs and wrote the manuscript.

Acknowledgements

We thank the broader communities working on GKLS dynamics, information geometry and stochastic gravity for foundational insights.

Gallardo VM (2026) The Universal Refined Equation (CUP-?*): Covariant GKLS Dynamics, Tomonaga–Schwinger Integrability, and Ein stein–Langevin Coupling in the CUCE/Spinoza/Hilbert Framework. J Phys Appl and Mech 3(1): 1016.

Received : 23 Dec 2025
Accepted : 20 Jan 2026
Published : 21 Jan 2026
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