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Unied Time Scale and Time Geometry: Causal Ordering, Unitary Evolution, and Generalized Entropy Haobo Ma 1 Wenlin Zhang 2 1 Independent Researcher 2 National University of Singapore November 20, 2025 Abstract We propose a unied time scale equivalence class rigorously gluing three ends of relativity, quantum scattering, and informationholography. Core scale identity unies derivative of total scattering phase, relative state density, and trace of WignerSmith group delay as dierent projections of same object: φ′(ω) π=ρrel(ω) = 1 2πtr Q(ω), Q(ω) = −iS(ω)†∂ωS(ω), φ =1 2arg det S. In geometry end, Killing time, ADM lapse, null geodesic ane parameter, and FRW conformal time proven mutually rescalable within unied equivalence class; in informationholography end, taking TomitaTakesaki modular ow as intrinsic time, controlling generalized entropy extremality on small causal diamonds with QFC/QNEC and relative entropy monotonicity, thus deriving Einstein equations in semiclassicalholographic window. Framework obtains three alignments: (i) phase proper time equivalence ϕ= (mc2/ℏ)Rdτ ; (ii) gravitational time delay = group delay trace ∆T=∂ωΦ = Tr Q ; (iii) FRW redshift = phase rhythm ratio 1 + z=a(t0)/a(te) = [(dϕ/dt)e]/[(dϕ/dt)0] . This paper under three axioms of causal orderingunitary evolutionentropy monotonicity/extremality , establishes existence and ane uniqueness of unied time scale, giving realization schemes for experimental and engineering metrology. Keywords: Time Geometry; Unied Time Scale; WignerSmith Group Delay; Spectral Shift Function; Killing/ADM/Null/Conformal/Modular Time; Generalized Entropy; QFC/QNEC MSC 2020: 83C45, 81U40, 81T20, 83C57 1 Introduction and Historical Context Role of time splits in dierent theories: general relativity scales causal structure with proper time, quantum theory generates unitary evolution with external parameter, information holography views modular ow as intrinsic thermal time. Yet when three end readings 1
synchronize, still lacking rigorous and metrologically measurable common scale. Wigner and Smith introduced derivative of phase with respect to energy in scattering theory dening time delay, trace of WignerSmith group delay matrix Q=−iS†∂ωS equals derivative of total phase Φ = arg det S , making idea of time = phase gradient rst land on experimentally readable ruler. BirmanKren formula characterizing state density change caused by interaction with spectral shift function tightly connects phase of scattering determinant with spectral geometry, thus deriving phase derivative = relative state density. In relativity side, redshift/clock rate in static spacetime given by gtt or Tolman Ehrenfest law; lapse N in ADM (3+1) decomposition characterizes ratio of coordinate time to proper time; tortoise coordinates and (u, v) in asymptotically at exterior provide natural null time at innity; in FRW cosmology 1+z=a(t0)/a(te) linearizes null geodesics with conformal time. In informationholography side, TomitaTakesaki modular theory endows any (state, algebra) pair with family of intrinsic one-parameter automorphisms (modular ow); ConnesRovelli thermal time hypothesis views this modular ow as physical time candidate; relative entropy monotonicity, QFC, and QNEC bind changes of generalized entropy together with stress tensor constraints, connecting to eld equations and reconstruction in small causal diamond limit. Above historical threads suggest: unifying phasegroup delayspectral shift with clock rateredshiftane/conformal time and modular timegeneralized entropy into single scale , hopeful to obtain cross-scale timegeometry framework. 2 Model and Assumptions (A) Causal and Global Structure Let (M, g) be stably causal Lorentzian manifold; under global hyperbolicity condition there exist smooth time function and smooth decomposition M∼ =R×Σ . (B) Scattering and Spectral Shift On absolutely continuous spectral energy window I⊂R , scattering matrix S(ω) unitary and smooth; dene total phase Φ = arg det S , group delay Q=−iS†∂ωS . There exists spectral shift function ξ(ω) and relative state density ρrel =−ξ′ ; BirmanKren formula det S(ω) = exp[−2πi ξ(ω)] holds. (C) Unied Scale Identity (Core Assumption) φ′(ω) π=ρrel(ω) = 1 2πtr Q(ω), φ =1 2Φ. (D) Boundary Entropy and Modular Flow Take small causal diamond Dp,r through point p , null generator ane parameter λ ; generalized entropy Sgen(λ) = Area(Σλ) 4Gℏ+Sout(λ) satises QFC/QNEC type inequalities and relative entropy monotonicity; modular Hamiltonian K=−ln ρ generates modular ow σs . (E) Unitary Evolution On state space H there exists strongly continuous unitary group U(t) = e−iHt ; semiclassical worldline limit can relate t and τ through phase density (see Section 4.1). 2
3 Unied Time Scale: Denition and Three Axioms 3.1 Unied Time Scale Equivalence Class Denition 3.1 (Unied Time Scale (Denition 3.1)) . There exists equivalence class [T]∼ {τ, t, tK,(N, Ni), λnull, u, v, η, ω−1, z, smod}, whose members mutually convertible through monotonic rescaling and geometric/entropy structure, making dynamics local, causally ordered, and entropy structure simplest. 3.2 Three Axioms Axiom 3.1 (Causal Ordering (Axiom I)) . In local hyperbolic domain there exists strictly increasing time function, making fundamental equations local (hyperbolic/rst-order) form. Axiom 3.2 (Unitary Evolution (Axiom II)) . There exists strongly continuous unitary group U(t) ; in semiclassical limit phasetime relation determined by Lagrangian stationary phase (Section 4.1). Axiom 3.3 (Entropy Monotonicity/Extremality (Axiom III)) . Along null cut family {Σλ} , Sgen satises relative entropy monotonicity and QFC/QNEC monotonicity/convexity and takes extremum under physical evolution; modular ow parameter s makes organization law of Sgen simplest. Theorem 3.1 (Mutual Implication in SemiclassicalHolographic Window (Theorem 3.2)) . Under small causal diamond limit and relative entropy monotonicity/QNEC holding: Axiom I + Axiom II ⇐⇒ Scale Identity =⇒ Axiom III =⇒ Einstein Equations . Proof in Section 5 and Appendices D/E. 4 Main Results (Theorems and Alignments) 4.1 PhaseProper Time Equivalence Theorem 4.1 (Worldline Principal Phase (Theorem 4.1)) . For narrow wave packet of mass m , in semiclassical limit ϕ=−1 ℏS[γcl] = mc2 ℏZγcl dτ, dϕ dτ=mc2 ℏ. (Proof: worldline path integral stationary phase; see Appendix B.) 4.2 Gravitational Time Delay = Group Delay Trace Theorem 4.2 (EikonalScattering Alignment (Theorem 4.2)) . In geometric optics limit of static or asymptotically at background, ∆T(ω) = ∂ωΦ(ω) = Tr Q(ω). Weak eld limit returns to Shapiro delay. 3
4.3 Redshift = Phase Rhythm Ratio Proposition 4.3 (FRW Phase Expression (Proposition 4.3)) . Under at FRW metric comoving observers measure 1 + z=νe ν0 = dϕ dte dϕ dt0 =a(t0) a(te). (See Appendix C.) 4.4 Four Bridges of GR Time Structure Bridge B (Killing TimeClock RateRedshift) In static metric ds2=−V(x)c2dt2+ ··· stationary observers have dτ=√Vdt , √V is local redshift/clock rate factor (Tolman Ehrenfest). Bridge C (ADM LapseLocal Clock Rate) ADM decomposition ds2=−N2dt2+ hij(dxi+Nidt)(dxj+Njdt) ; Euler family orthogonal to slicing satises dτ=Ndt . Bridge D (Null Ane ParameterRetarded/Advanced/Conformal Time) Asymptotically at exterior denes tortoise r∗ and u=t−r∗, v =t+r∗ , monotonically equivalent to null geodesic ane parameter; in FRW dη= dt/a(t) linearizes null geodesics. Bridge E (Modular TimeEntropy GradientGeometric Equations) Parameter s of modular ow σs provides information-theoretic time; relative entropy monotonicity and QNEC/QFC bind extremality/monotonicity of ∂sSgen with ⟨Tkk⟩ . 4.5 Entropic Geometric Form of Einstein Equations Theorem 4.4 (EntropyGeometry (Theorem 4.4)) . Under Axiom III and Raychaudhuri equation, on small causal diamond have Rµν −1 2Rgµν + Λgµν = 8πG ⟨Tµν⟩. (Proof: combining second-order area variation with QNEC/relative entropy, see Appendix D; cf. Jacobson and subsequent holographic arguments.) 4.6 Unied Scale Identity (SpectralScatteringGeometry) Corollary 4.5 (Corollary 4.5) . φ′(ω) π=ρrel(ω) = 1 2πtr Q(ω), obtained by combining BirmanKren and Tr Q=∂ωΦ (Appendix A). 4
5 Proofs (Key Points) 5.1 Theorem 4.1: Worldline action stationary phase along timelike geodesic, uctuations only change quantum prefactor, principal phase gives ϕ= (mc2/ℏ)Rdτ (Appendix B). 5.2 Theorem 4.2: Eikonal phase dierence ∆S≃ −ℏω∆T aligns with scattering ∂ωΦ = Tr Q , yielding ∆T= Tr Q ; weak eld test returns to Shapiro delay. 5.3 Proposition 4.3: Null geodesic and scale factor give ν∝1/a(t) , redshift as phase rhythm ratio (Appendix C). 5.4 Bridges BE: Static clock rate, ADM lapse, null coordinates, and modular ow each consistent with standard conclusions and literature (Appendix E). 5.5 Theorem 4.4: Raychaudhuri's second-order area variation ∝ −RRkk combines with QNEC S′′ out ≥(2π/ℏ)R⟨Tkk⟩ , extremality condition S′ gen(0) = 0 yields tensor equation (Appendix D); QFC provides stronger monotonicity background. 6 Model Applications A. Frequency-Domain Reconstruction of Solar System Geometric Delay Differentiating multi-frequency radar echo phase Φ(ω) gives ∆T(ω) = ∂ωΦ = Tr Q , compare with Shapiro delay, can parallelly strip plasma dispersion term. B. PhaseGroup Delay Unication of Gravitational Lensing Image pair (i, j) Fermat potential dierence ∆tij equals ∂ω[Φi−Φj] ; broadband electromagnetic/gravitational wave joint use for Hubble constant and mass model systematic error suppression. C. Cosmological Phase Ruler Directly estimate a(t) using phase rhythm ratio of pulsar/FRB, avoiding specic spectral line systematics; phaseredshift synchronization guaranteed by Proposition 4.3. D. Eective Time Refractive Index Tomography Invert nt= (−gtt)−1/2 from spatial distribution of ρrel(ω) or tr Q(ω) , cooperating with optical metricFermat principle for weak eld time delay imaging. 7 Engineering Proposals 1. On-chip group delay tomography metrology: Measure S(ω) in integrated photonics and real-time compute Tr Q(ω) , generating equivalent gravitational time delay map for device inversion and robust design. 2. Double-height matter wave standard: COW geometric arrangement compare ∆ϕ and ∆τ , test linear regime of ∆ϕ= (mc2/ℏ)∆τ . 3. Broadband lens group delay spectrum: Synchronously t each image arrival time delay and dispersion using ∂ωΦ , reducing time delay cosmology systematic errors. 4. Entropy light cone platform: Measure second-order deformation and energy ow of Sout on controllable quantum system, test QNEC/QFC coecients and saturation conditions. 5
8 Discussion (Risks, Boundaries, Past Work) (i) Spectral endpoints and regularity: Scale identity requires S(ω) dierentiable and belonging to appropriate determinant class; near resonances and thresholds need contour displacement and trace-class regularization. (ii) Geometric optics and strong elds: Strong spin/non-static backgrounds need generalized optical metric and coherent transport; near-horizon regions better use null coordinates and numerical ray tracing. (iii) Entropygeometry assumption domain: QNEC has general QFT proofs and holographic proofs continuously strengthening (including latest new proof approaches), but still advancing in high curvature, strong quantum gravity regions. (iv) GR time structure unication: Killing/ADM/null/conformal/modular times are coordinatizations of unied scale in dierent projections; BernalSánchez's global time functions and ADM foliation provide rigorous foundation. 9 Conclusion Under three axioms of causal orderingunitary evolutionentropy monotonicity/extremality , obtain unied time scale equivalence class, aligning microscopic (phase/scattering), mesoscopic (group delay/redshift), and macroscopic (entropygeometry) three-end languages. Core conclusions: ϕ=mc2 ℏZdτ, ∆T(ω) = ∂ωΦ(ω) = Tr Q(ω),1+z=(dϕ/dt)e (dϕ/dt)0 , Gµν+Λgµν = 8πG ⟨Tµν⟩, and spectralscatteringgeometry scale identity φ′/π =ρrel = (2π)−1tr Q . Time thus can be characterized as: equivalence class of one-dimensional parameter making dynamics local, causality clear, entropy structure simplest ; its dierent names merely coordinates of same object in dierent projections. Acknowledgements, Code Availability Thanks to related textbooks and literature. Symbolic derivations and numerical scripts for group delaytime delay reconstruction and FRW phase rhythm demonstration available upon request. References [1] E. P. Wigner, Lower Limit for the Energy Derivative of the Scattering Phase Shift, Phys. Rev. 98 (1955) 145. 6
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A WignerSmith Group Delay and SpectralScattering Geometry Identity A.1 BirmanKren and Spectral Shift For self-adjoint pair (H, H0) with trace-class/quasi-trace-class perturbation, spectral shift function ξ(ω) satises det S(ω) = e−2πiξ(ω)⇒1 2π∂ωΦ(ω) = −ξ′(ω) = ρrel(ω). (See reference 3.) A.2 Trace Identity From Q(ω) = −iS†∂ωS and Tr ln S= ln det S obtain Tr Q(ω) = ∂ωΦ(ω). Combining A.1 gives scale identity: φ′(ω) π=ρrel(ω) = 1 2πtr Q(ω). B PhaseProper Time Under Worldline Path Integral Fermi normal coordinate expansion along timelike geodesic γcl S[γ] = −mc2Zdτ+m 2Zdτ δij ˙yi˙yj+··· . Stationary phase gives ϕ=−1 ℏS[γcl] = mc2 ℏZdτ, dϕ dτ=mc2 ℏ. C Phase Expression of Redshift in FRW Cosmology Flat FRW: ds2=−dt2+a(t)2dx2 . Comoving observer uµ= (1,0,0,0) , photon eikonal phase ϕ has kµ=∂µϕ and ν=−1 2πkµuµ=1 2π dϕ dt∝1 a(t)⇒1 + z=(dϕ/dt)e (dϕ/dt)0 =a(t0) a(te). (Reference 7.) 8
D Generalized Entropy Extremality/Monotonicity and Field Equations Let {Σλ} be null cut family through p . Raychaudhuri: ˙ θ=−1 2θ2−σ2−Rkk . Second-order area variation d2A/dλ20∝ −ZRkk dA . QNEC and relative entropy monotonicity: d2Sout/dλ20≥2π ℏZ⟨Tkk⟩dA . Extremum S′ gen(0) = 0 combines to give Rkk = 8πG⟨Tkk⟩ , holding for any kµ , upgrades to tensor equation and gives Λ as integration constant. E Renement of GR Time Bridges E.1 Static Spacetime (Killing): ξµ is timelike Killing vector, stationary observer uµ=ξµ/p−ξ2 , if gtt =−V then dτ=√Vdt . (TolmanEhrenfest temperature redshift law same form.) E.2 ADM Lapse: ds2=−N2dt2+hij(dxi+Nidt)(dxj+Njdt) ; slicing orthogonal family satises dxi+Nidt= 0 ⇒dτ=Ndt . E.3 Null Coordinates: Schwarzschild exterior r∗=r+2Mln |r/2M−1| , u=t−r∗ , v=t+r∗ ; in FRW dη= dt/a(t) . E.4 Modular Time: Given (algebra, state) pair (A, ω) GNS representation, modular ow σs intrinsically denes time; under half-space and small deformations, K localizes to RTkk , isomorphic with ANEC/QNEC, JLMS/relative entropy. F Shapiro Delay and Group Delay Weak eld Schwarzschild exterior ∆t≃4GM c3ln 4rErR b2+··· , consistent with frequency-domain measured ∂ωΦ = Tr Q ; multi-frequency echo tting can separate dispersion and geometric terms. G Existence and Uniqueness of Unied Time Scale Given scattering data (S(ω)) satisfying scale identity. Dene t−t0=Zω ω0 1 2πTr Q(˜ω) d˜ω=Zω ω0 φ′(˜ω) πd˜ω=Zω ω0 ρrel(˜ω) d˜ω. In non-degenerate frequency window derivative positive, t(ω) locally bijective; if another ˜ t satises same condition, then ˜ t=at +b ( a > 0 ), giving ane uniqueness. 9