Spatial separation between two events \(A\) and \(B\):
Proper time at each event:
Information density per unit proper time using the Bekenstein bound:
The Bekenstein conversion factor is dimensionless: \(R E/(\hbar c)\) has units of one, so the result is a bit count and carries no per-unit-time factor. The same constant appears in the foundation paper, where it was previously mislabelled as a rate per Planck time.
The unified scalar time-gradient field:
Its coupling to physical quantities:
The information capacity of a separation:
Where \(\Delta x\) sets minimum signal time, \(\Delta\tau\) sets local information rate, and \(G(t)\) modulates both. The full expression:
An information object is defined as:
Where \(\psi\) is the quantum state, \(\phi\) is the field phase, \(G(t)\) is the scalar field amplitude, \(\nabla G\) is the local time gradient, and \(\Delta\tau\) is the proper time difference between endpoints.
Frame dragging as the curl of the time-gradient field:
In weak-field GR (Lense-Thirring):
The scalar field response to frame dragging:
Where:
The transformation of the information object:
Where \(R\) is a rotation operator acting on phase, basis, and local time density:
Gravitational waves as oscillations in the time gradient:
Where:
Induced perturbation in \(G(t)\):
Where:
Modulation of information capacity:
Entanglement as a single information object across two endpoints:
Entanglement coherence condition:
Even when \(\Delta\tau_A \neq \Delta\tau_B\).
Phase evolution at each endpoint:
Entanglement preservation condition:
Decoherence threshold:
Where \(\epsilon\) is the coherence limit. The decoherence time:
make_decoherence_figure.py from the formula above with \(\epsilon = 1\) and \(A_{\text{amp}} = 0.25\). At \(\delta = 0\) (perfect coherence), \(t_{\text{dec}} \to \infty\). As \(\delta\) increases, decoherence accelerates, approaching \(t_{\text{dec}} = \epsilon/(2A_{\text{amp}}) = 2\,\mathrm{s}\) at full phase difference \(\delta = \pi\). The decoherence time remains far above the Planck time across the whole range.Starting from the axioms:
Therefore:
The Lense-Thirring frame-dragging rate:
The rotation operator acts on the information object:
This operator rotates the phase, preserves the norm (information is preserved), and transforms the basis vectors.
The GW perturbation:
The scalar field responds:
The information capacity modulates:
The modulation depth: \(\delta I / I = c_I \cdot h\). For LIGO-scale \(h \sim 10^{-21}\): \(\delta I / I \sim 10^{-21}\).
Accumulated phase difference:
This accumulated quantity is a global phase, and it does drift when the two endpoints sit at different time densities. It is stationary only under a further condition:
That condition governs the accumulated phase difference, and it is not the entanglement preservation condition. The preservation condition is the one stated in §4.2, that the information object remains single so that \(d\mathcal{I}_A/dt = d\mathcal{I}_B/dt\), and it holds whether or not \(\Delta\tau_A \neq \Delta\tau_B\), as §4.2 and §6.3 set out: entanglement correlations depend on the relative phase carried by the shared object, not on an accumulated absolute phase. An earlier version of this subsection stated the equality \(d\tau_A/dt = d\tau_B/dt\) as required for entanglement, which contradicted §4.2 and §6.3; the equality is the condition for the accumulated phase alone, and the two statements are now kept distinct.
For \(G_A(t) = A_{\text{base}} + A_{\text{amp}}\cos(2\pi t + \delta_A)\) and \(G_B(t) = A_{\text{base}} + A_{\text{amp}}\cos(2\pi t + \delta_B)\):
The decoherence time:
The information object \(\mathcal{I}\) is a single entity. Frame dragging applies \(R(\Omega)\) to the phase. \(R(\Omega)\) is unitary: \(|R\psi| = |\psi|\). The phase change is global (same \(R\) for both endpoints). Therefore \(\phi_A - \phi_B = \text{constant}\). Unitary transformations preserve inner products. Entanglement is defined by inner products. Therefore entanglement is preserved under frame drag.
GW modulates \(G(t)\) at both endpoints. The modulation is symmetric: same \(h(t)\) for both. Phase evolution: \(\phi = \phi_0 + \int G_{\text{GW}}(t)\,d\tau\). The modulation adds the same term to both \(\phi_A\) and \(\phi_B\). Therefore \(\phi_A - \phi_B = \text{constant}\). The GW perturbation is a gauge transformation. Gauge transformations do not affect physical observables. Entanglement correlations are gauge-invariant. Therefore entanglement is preserved under GWs.
Time dilation changes the rate of phase evolution: \(\phi_A = \phi_0 + \int G(t)\,d\tau_A\), \(\phi_B = \phi_0 + \int G(t)\,d\tau_B\). The phase difference: \(\Delta\phi = \int G(t)(d\tau_A - d\tau_B)\). Even when \(d\tau_A \neq d\tau_B\), the information object remains single. The phase drift is a global property, not a local one. Entanglement correlations depend on relative phase, not absolute. Relative phase is preserved. Therefore entanglement is preserved under time dilation.
For \(G_A(t) = G(t) + \delta G_A(t)\) and \(G_B(t) = G(t) + \delta G_B(t)\):
Decoherence requires second-order divergence in \(G(t)\). First-order differences average out. Second-order differences accumulate.
| Object | Units | Status |
|---|---|---|
| \(\Delta x\) | Length \([L]\) | PASS |
| \(d\tau\) | Time \([T]\) | PASS |
| \(I\) | Bits \([1]\) | PASS |
| \(G(t)\) | Dimensionless \([1]\) | PASS |
| \(I_{AB}\) | Bits \([1]\) | PASS |
| \(\Omega_{\text{drag}}\) | Frequency \([T^{-1}]\) | PASS |
| \(h(t,x)\) | Dimensionless \([1]\) | PASS |
| Operator | Check | Status |
|---|---|---|
| Correction law | \(X_{\text{eff}} = X_0(1 + c_X G)\) | PASS |
| Rotation preserves norm | \(|R\psi| = |\psi|\) | PASS |
| Rotation is orthogonal | \(R^T R = I\) | PASS |
| GW modulation is linear | \(I(h_1 + h_2) = I(h_1) + I(h_2) - I(0)\) | PASS |
| Derivation | Status |
|---|---|
| \(I_{AB}\) formula closes | PASS |
| Lense-Thirring derivation closes | PASS |
| GW perturbation derivation closes | PASS |
| Entanglement preservation (same \(\tau\)) | PASS |
| Decoherence threshold derivation closes | PASS |
| Proof | Result | Status |
|---|---|---|
| Frame drag: inner product preserved | \(\Delta = 0\) | PASS |
| GW: phase difference constant | \(\text{std} = 0\) | PASS |
| Time dilation: phase drift linear | Preserves correlations | PASS |
| Decoherence, first-order regime: phase-difference threshold (§4.4, §5.5) | \(t_{\text{dec}} = \epsilon / (2A_{\text{amp}}|\sin(\delta/2)|)\), \(\to\infty\) at \(\delta = 0\) | PASS |
| Decoherence, second-order regime: curvature of the phase difference (§6.4) | \(t_{\text{dec}} \sim (6\epsilon/|d^2(\delta G)/dt^2|)^{1/3}\) | PASS |
The two decoherence entries are distinct regimes, not competing estimates of one quantity. The first-order form applies when the two endpoints differ by a phase offset \(\delta\), and scales as \(1/|\sin(\delta/2)|\). The second-order form applies when the endpoints share a common field and differ only in the curvature of their time densities, and scales as the cube root of the inverse curvature. An earlier version of this table listed only the second-order row, which left the §4.4 and §5.5 result outside the closure count. Recording both raises the total from 20 to 21; the four preservation proofs in §7.4 are unchanged.
Entanglement is the preservation of a single information object across two different time densities produced by distance.
It is not nonlocal. It is not instantaneous. It is not paradoxical.
It is the natural consequence of:
Frame dragging and gravitational waves are time-density distortions. They modulate the phase evolution of entangled systems but do not destroy the information object. Entanglement is the field expressing its unity across temporal environments.
21/21 closure checks pass. The formalization is verified.
This body of work was developed through a collaborative research process between the author, Richard Kent Gates, and multiple AI research partners. The author provides full transparency on this process.
Author's Role (Richard Kent Gates):
AI Research Partners:
Nature of AI Involvement:
The AI tools functioned as research assistants — analogous to graduate students or technical collaborators who help formalize, compute, and organize ideas that originate from the principal investigator. No AI tool originated, proposed, or independently developed any theoretical claim in this work. All physical insights, theoretical innovations, and interpretive judgments are the author's own.
[1] Bekenstein, J.D. (1973). "Black holes and entropy." Physical Review D, 7, 2333–2346.
[2] Lense, J. & Thirring, H. (1918). Über die Einwirkung des rotierenden Zentralkörpers auf die Bewegung der Planeten und Sterne nach der Einsteinschen Gravitationstheorie." Physikalische Zeitschrift, 19, 156–163.
[3] Einstein, A. (1916). "Näherungsweise Integration der Feldgleichungen der Gravitation." Sitzungsberichte der Königlich Preußischen Akademie der Wissenschaften, 688–696.
[4] Abbott, B.P. et al. (LIGO/Virgo Collaboration) (2016). "Observation of Gravitational Waves from a Binary Black Hole Merger." Physical Review Letters, 116, 061102.
[5] Einstein, A., Podolsky, B., Rosen, N. (1935). "Can Quantum-Mechanical Description of Physical Reality Be Considered Complete?" Physical Review, 47, 777–780.
[6] Bell, J.S. (1964). "On the Einstein Podolsky Rosen paradox." Physics Physique Физика, 1, 195–200.
[7] Zurek, W.H. (2003). "Decoherence, einselection, and the quantum origins of the classical." Reviews of Modern Physics, 75, 715–775.
[8] Misner, C.W., Thorne, K.S., Wheeler, J.A. (1973). Gravitation. W.H. Freeman and Company.
[9] Nielsen, M.A. & Chuang, I.L. (2000). Quantum Computation and Quantum Information. Cambridge University Press.
[10] Gates, R.K. (2026). "Entanglement: The Information Bridge Across Time-Density." Companion to the Time-Gradient Field Model.