Unified Informational Theory: From Quantum Phase Information to Physical Records in Spacetime, from Relativity to the Forces

What if time is not a dimension you move through, but a ledger you write into? To feel one moment come after another, something must be remembered. No memory, no past, no future: only an undifferentiated present. Memory is the sense organ of time, the way the eye is the sense organ of a narrow band of the electromagnetic field. What we, and every other memory bearing systems, experience as the flow of time is the ordered comparison of written records. And a record is written information: physical, countable, and work-coupled. Irreversible stabilization, reset, overwrite, or loss of access carries Landauer’s bill. But the phase beneath the record turns freely and writes nothing. Take that distinction seriously, free reversible phase beneath thermodynamically paid irreversible record boundaries, and follow it with discipline. Something unexpected happens: the forces of nature stop looking like separate ingredients and start looking like different readings of one object, all using one phase-rate currency. One typed law: ΔE = ħΔΩ, with spatial gradient, state-space derivative, or connection curvature selected by the branch.One budget: χ² + Λ = 1 One invariant mass cadence: ω_C = mc²/ħ GRAVITY: ΔΩ_g = ω_C = m·(χ_g − 1), χ_g = √(1 − r_s/r)recovers Newtonian attraction in the weak-field limit and the Schwarzschild exterior as the static spherical capacity readout. INERTIA: U_χ,v = ħω_Cχ_v = mc²χ_v, χ_v = 1/γ, with p = −∂U_χ,v/∂v = γmv as the kinematic readout and F = dp/dt as its reconfiguration response. The Lorentz factor appears as an allocation receipt, not as a primitive geometry postulate. DIFFUSION: ΔΩ_D = Ω_ref·[1 − χ_D(n, η_I, E_env)] yields Fick’s law with the correct Einstein coefficient D_diff = bk_BT. ENTROPY: Ṡ_mono,m/k_B = Ī_mono,m^nat = ω_Cevery mass carries monotonic entropy at its own Compton rate, or ω_C/ln2 in bits per unit parameter time. This is not heat by itself. It is monotonic throughput: from a warm gas, mc²(1 − ⟨χ_v⟩) ≃ 3/2 k_BT, to the black-hole horizon, S = k_B·A/4ℓ_P². ELECTRICITY: Ξ_EM(r) = ΔΩ_EM/ω_C = α·(λ̄_C/r) yields Coulomb: U_Coul = αħc/r,F_Coul = αħc/r². Charge is integer winding of the compact phase-transport sector, which is why charge is quantized and signed while mass is continuous and positive. MAGNETISM:|A_∥|/(V′_em/c), γβ = tan θ_v = p/(mc), together with dp/dt = q(E + v × B), yields the magnetic companion of the electric phase connection, with the mixing coefficient tan θ_v = γβ obtained twice, from independent routes. WEAK: ΔΩ_W = ω_tr·Λ_W^(φ), with Λ_W^(φ) = ε_W·a_W·(1 − cos φ_W). The weak readout is the record-space projection of a finite phase-time orientation gradient: F_W^reg = −ħω_tr ∇_reg[ε_W·a_W·(1 − cos φ_W)]≃ −ħω_tr ε_W·a_W·sinφ_W ∇_regφ_W. This is the ledger’s mandatory inverse: local unwriting of an identity record. The primary weak rate law remains Γ_dec = τ_0^−1 2^−ΔI_w^bit, with a citation-anchored taxonomy of environment-dependent nuclear half-life shifts and strict prohibitions where no reconstruction handle exists. STRONG: the strong sector is a zero-sum closure of three phase carriers in the complex phase plane: z_a = a_a e^(iφ_a), a = 1,2,3, z_1 + z_2 + z_3 = 0. For equal amplitudes, the symmetric closure is separated by 120 degrees: 1 + e^(2πi/3) + e^(4πi/3) = 0. Each carrier retains positive energy, while their directed complex phase sum cancels. Any local amplitude change, relative-phase displacement, or deformation breaks the closure: Δz = z_1 + z_2 + z_3 ≠ 0. The resulting closure energy and restoring force are V_local = (κ_cl/2)|Δz|², ΔΩ_local = V_local/ħ, F_a = −∇_(ξ_a)V_local = −ħ∇_(ξ_a)ΔΩ_local. Thus the strong force is the restoring response to any nonzero gradient of three-carrier phase misclosure. At large separation, the unresolved phase mismatch accumulates along the connecting path and produces the linear confinement branch σr. At short distance, non-Abelian connection exchange supplies the Coulombic branch, so the established convergence target is V_Cornell(r) = −C_F α_s(r)ħc/r + σr + V_0. The same three-carrier architecture gives the traceless rearrangement count 3 × 3 − 1 = 8 = 6 + 2, and the external real projection weights 1/3 and 2/3, while the full QCD coupling, running, string tension, and spectrum remain the quantitative completion target. One phase-rate currency, ΔE = ħΔΩ, in every row.One typed response principle on it.Eight established landmarks out.Only the sectoral load, connection, orientation, or closure variable changes. The table appears on page 2, before a single derivation, so the unification is visible before the argument begins. SIX EMPIRICAL AND STRUCTURAL WAYS TO TEST OR BREAK IT Every claim in the paper carries an inline epistemic tag: what is imported from established physics, what is derived, what is interpretation, what is calibration, and what is honestly open. The framework’s own exposure is concentrated in six empirical or structural commitments. Five define identifiable laboratory or observational programs. The fifth is a quantitative structural-completion test. I. CLOSED-LOOP RECORD UNWRITING. A controlled write-then-unwrite loop must restore the pre-record physical state and close the declared reversible work ledger. The reversal must include the event, memory, environmental support, controls, and work reservoir. The forward registration and Landauer-bound components are already experimentally established; the complete closed loop is targetable on trapped-ion and superconducting platforms. Failure to restore both the state and the full energy ledger breaks the record-unwriting theorem. II. GRAVITY CHANNEL TYPING. The framework predicts a strict null for gravitationally mediated mass-mass entanglement in Bose-Marletto-Vedral-type experiments. Static gravity is assigned to a coherent monotonic-capacity channel rather than a branch-specific configurational channel. A single controlled positive entanglement result attributable to gravity kills this two-channel assignment outright. III. DRIVEN COHERENT PHASE TRANSPORT. A phase-selective drive above the equilibrium critical temperature must increase coherent phase stiffness more strongly than dissipative spectral weight. The decisive classifier is the ratio of coherent to dissipative response under matched driven, thermal, and broad-spectrum controls. Driven cuprates, fullerides, and related materials already provide the experimental arena. Heating-only outcomes under genuinely phase-selective driving count against the framework. IV. WEAK REWRITE TAXONOMY. Decay by decay, the framework predicts which environmental handle can alter a rate, which sign the change must have, and which decay classes must remain stable. The prediction is fixed by the daughter-record requirement and the reverse-reconstruction path. Confirmed examples already include electron-density effects in electron capture, bound-state beta decay in highly ionized atoms, and sign-resolved hyperfine effects. A confirmed modulation with no identified reconstruction handle, or a robust sign opposite to the pre-registered daughter-slot prediction, breaks the taxonomy. V. STRONG CLOSURE GEOMETRY. The three-carrier closure must be completed into quantitative non-Abelian dynamics. The completed action must recover color-blind electric charge, SU(3) transport, the eight gauge directions, running coupling, confinement, string tension, singlet structure, and the observed hadron spectrum. This is a structural completion test rather than a single laboratory experiment. Failure to recover those quantitative structures kills the strong-sector claim. VI. QUADRATIC PHOTON ARRIVAL-TIME SCALING. After source-intrinsic, plasma, conventional gravitational, cosmological, and instrumental delays are modeled, the universal propagation residual must scale quadratically with photon energy: Δt_γ ∝ E_γ², with zero universal linear term and the predicted cosmological redshift integral. Existing high-energy transient observations already constrain both linear and quadratic dispersion. A confirmed universal linear vacuum-dispersion term breaks the framework.

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Publication Details

Journal
Zenodo (CERN European Organization for Nuclear Research)
Published
2026-07-22
DOI
https://doi.org/10.5281/zenodo.21495321
Primary Topic
Quantum Mechanics and Applications
Type
preprint
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preprint

Unified Informational Theory: From Quantum Phase Information to Physical Records in Spacetime, from Relativity to the Forces

yaniv riz
Zenodo (CERN European Organization for Nuclear Research)
Quantum Mechanics and Applications
preprint

Unified Informational Theory: From Quantum Phase Information to Physical Records in Spacetime, from Relativity to the Forces

yaniv riz
preprint en

Abstract

What if time is not a dimension you move through, but a ledger you write into? To feel one moment come after another, something must be remembered. No memory, no past, no future: only an undifferentiated present. Memory is the sense organ of time, the way the eye is the sense organ of a narrow band of the electromagnetic field. What we, and every other memory bearing systems, experience as the flow of time is the ordered comparison of written records. And a record is written information: physical, countable, and work-coupled. Irreversible stabilization, reset, overwrite, or loss of access carries Landauer’s bill. But the phase beneath the record turns freely and writes nothing. Take that distinction seriously, free reversible phase beneath thermodynamically paid irreversible record boundaries, and follow it with discipline. Something unexpected happens: the forces of nature stop looking like separate ingredients and start looking like different readings of one object, all using one phase-rate currency. One typed law: ΔE = ħΔΩ, with spatial gradient, state-space derivative, or connection curvature selected by the branch.One budget: χ² + Λ = 1 One invariant mass cadence: ω_C = mc²/ħ GRAVITY: ΔΩ_g = ω_C = m·(χ_g − 1), χ_g = √(1 − r_s/r)recovers Newtonian attraction in the weak-field limit and the Schwarzschild exterior as the static spherical capacity readout. INERTIA: U_χ,v = ħω_Cχ_v = mc²χ_v, χ_v = 1/γ, with p = −∂U_χ,v/∂v = γmv as the kinematic readout and F = dp/dt as its reconfiguration response. The Lorentz factor appears as an allocation receipt, not as a primitive geometry postulate. DIFFUSION: ΔΩ_D = Ω_ref·[1 − χ_D(n, η_I, E_env)] yields Fick’s law with the correct Einstein coefficient D_diff = bk_BT. ENTROPY: Ṡ_mono,m/k_B = Ī_mono,m^nat = ω_Cevery mass carries monotonic entropy at its own Compton rate, or ω_C/ln2 in bits per unit parameter time. This is not heat by itself. It is monotonic throughput: from a warm gas, mc²(1 − ⟨χ_v⟩) ≃ 3/2 k_BT, to the black-hole horizon, S = k_B·A/4ℓ_P². ELECTRICITY: Ξ_EM(r) = ΔΩ_EM/ω_C = α·(λ̄_C/r) yields Coulomb: U_Coul = αħc/r,F_Coul = αħc/r². Charge is integer winding of the compact phase-transport sector, which is why charge is quantized and signed while mass is continuous and positive. MAGNETISM:|A_∥|/(V′_em/c), γβ = tan θ_v = p/(mc), together with dp/dt = q(E + v × B), yields the magnetic companion of the electric phase connection, with the mixing coefficient tan θ_v = γβ obtained twice, from independent routes. WEAK: ΔΩ_W = ω_tr·Λ_W^(φ), with Λ_W^(φ) = ε_W·a_W·(1 − cos φ_W). The weak readout is the record-space projection of a finite phase-time orientation gradient: F_W^reg = −ħω_tr ∇_reg[ε_W·a_W·(1 − cos φ_W)]≃ −ħω_tr ε_W·a_W·sinφ_W ∇_regφ_W. This is the ledger’s mandatory inverse: local unwriting of an identity record. The primary weak rate law remains Γ_dec = τ_0^−1 2^−ΔI_w^bit, with a citation-anchored taxonomy of environment-dependent nuclear half-life shifts and strict prohibitions where no reconstruction handle exists. STRONG: the strong sector is a zero-sum closure of three phase carriers in the complex phase plane: z_a = a_a e^(iφ_a), a = 1,2,3, z_1 + z_2 + z_3 = 0. For equal amplitudes, the symmetric closure is separated by 120 degrees: 1 + e^(2πi/3) + e^(4πi/3) = 0. Each carrier retains positive energy, while their directed complex phase sum cancels. Any local amplitude change, relative-phase displacement, or deformation breaks the closure: Δz = z_1 + z_2 + z_3 ≠ 0. The resulting closure energy and restoring force are V_local = (κ_cl/2)|Δz|², ΔΩ_local = V_local/ħ, F_a = −∇_(ξ_a)V_local = −ħ∇_(ξ_a)ΔΩ_local. Thus the strong force is the restoring response to any nonzero gradient of three-carrier phase misclosure. At large separation, the unresolved phase mismatch accumulates along the connecting path and produces the linear confinement branch σr. At short distance, non-Abelian connection exchange supplies the Coulombic branch, so the established convergence target is V_Cornell(r) = −C_F α_s(r)ħc/r + σr + V_0. The same three-carrier architecture gives the traceless rearrangement count 3 × 3 − 1 = 8 = 6 + 2, and the external real projection weights 1/3 and 2/3, while the full QCD coupling, running, string tension, and spectrum remain the quantitative completion target. One phase-rate currency, ΔE = ħΔΩ, in every row.One typed response principle on it.Eight established landmarks out.Only the sectoral load, connection, orientation, or closure variable changes. The table appears on page 2, before a single derivation, so the unification is visible before the argument begins. SIX EMPIRICAL AND STRUCTURAL WAYS TO TEST OR BREAK IT Every claim in the paper carries an inline epistemic tag: what is imported from established physics, what is derived, what is interpretation, what is calibration, and what is honestly open. The framework’s own exposure is concentrated in six empirical or structural commitments. Five define identifiable laboratory or observational programs. The fifth is a quantitative structural-completion test. I. CLOSED-LOOP RECORD UNWRITING. A controlled write-then-unwrite loop must restore the pre-record physical state and close the declared reversible work ledger. The reversal must include the event, memory, environmental support, controls, and work reservoir. The forward registration and Landauer-bound components are already experimentally established; the complete closed loop is targetable on trapped-ion and superconducting platforms. Failure to restore both the state and the full energy ledger breaks the record-unwriting theorem. II. GRAVITY CHANNEL TYPING. The framework predicts a strict null for gravitationally mediated mass-mass entanglement in Bose-Marletto-Vedral-type experiments. Static gravity is assigned to a coherent monotonic-capacity channel rather than a branch-specific configurational channel. A single controlled positive entanglement result attributable to gravity kills this two-channel assignment outright. III. DRIVEN COHERENT PHASE TRANSPORT. A phase-selective drive above the equilibrium critical temperature must increase coherent phase stiffness more strongly than dissipative spectral weight. The decisive classifier is the ratio of coherent to dissipative response under matched driven, thermal, and broad-spectrum controls. Driven cuprates, fullerides, and related materials already provide the experimental arena. Heating-only outcomes under genuinely phase-selective driving count against the framework. IV. WEAK REWRITE TAXONOMY. Decay by decay, the framework predicts which environmental handle can alter a rate, which sign the change must have, and which decay classes must remain stable. The prediction is fixed by the daughter-record requirement and the reverse-reconstruction path. Confirmed examples already include electron-density effects in electron capture, bound-state beta decay in highly ionized atoms, and sign-resolved hyperfine effects. A confirmed modulation with no identified reconstruction handle, or a robust sign opposite to the pre-registered daughter-slot prediction, breaks the taxonomy. V. STRONG CLOSURE GEOMETRY. The three-carrier closure must be completed into quantitative non-Abelian dynamics. The completed action must recover color-blind electric charge, SU(3) transport, the eight gauge directions, running coupling, confinement, string tension, singlet structure, and the observed hadron spectrum. This is a structural completion test rather than a single laboratory experiment. Failure to recover those quantitative structures kills the strong-sector claim. VI. QUADRATIC PHOTON ARRIVAL-TIME SCALING. After source-intrinsic, plasma, conventional gravitational, cosmological, and instrumental delays are modeled, the universal propagation residual must scale quadratically with photon energy: Δt_γ ∝ E_γ², with zero universal linear term and the predicted cosmological redshift integral. Existing high-energy transient observations already constrain both linear and quadratic dispersion. A confirmed universal linear vacuum-dispersion term breaks the framework.

Zenodo (CERN European Organization for Nuclear Research)
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Quantum Mechanics and Applications
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