Geometric Origin of Quantum Entanglement from Worldline Non-Injectivity: Area Law, Decoherence, and Spacetime Connectivity

Abstract

What is the geometric origin of quantum entanglement? In standard quantum mechanics, entanglement is a postulate: composite systems occupy tensor product Hilbert spaces, and states need not factorize. Its emergence from deeper physical principles has remained an open question. This paper provides a rigorous answer: entanglement is a geometric consequence of worldline non-injectivity. The framework rests on a single kinematic fact established in the companion paper "Worldline Non-Injectivity as a Necessary and Sufficient Condition for the Emergence of Holographic Spacetime": when a massive body travels at ultra-relativistic velocities $\gamma \geq \gamma_{\text{crit}}$, its worldline $X^\mu(\tau)$ intersects the simultaneity foliation $\Sigma_t$ in $N > 1$ distinct spatial points. These $N$ intersections are not $N$ distinct particles, but $N$ temporal appearances of the same physical entity. The central achievement of this paper is the derivation of the **Ontological Identity Principle (OIP)** — the statement that all $N$ appearances are manifestations of one entity, and that the multi-sheet state is a coherent superposition with uniform coefficients $|c_n| = 1/\sqrt{N}$ — not as a postulate, but as a **theorem**. The proof rests on three independent lemmas, each grounded in results already established within the TPST–DGQ framework: 1. **Unitarity of proper-time transport (Lemma 1):** The continuity of the worldline $X^\mu(\tau) \in C^\infty(\mathbb{R})$ and the Hamiltonian structure of the theory imply that the evolution operator between proper times is unitary, forcing the total state to be a coherent superposition over all sheets. 2. **Topological superselection rule (Lemma 2):** No local physical observable can distinguish the $n$-th sheet from the $m$-th sheet without breaking the $C^\infty$ regularity of $X^\mu(\tau)$. Since no topological defect separates the sheets, there is no conserved quantum number capable of differentiating them, forbidding classical mixtures and enforcing quantum coherence. 3. **Permutation symmetry (Lemma 3):** The sheets are indistinguishable manifestations of the same entity, so the physics is invariant under any permutation $\sigma \in S_N$ of the sheet labels. The unique pure state invariant under the full permutation group $S_N$ is the uniform superposition with coefficients $|c_n| = 1/\sqrt{N}$. From this derived OIP, the paper obtains five major results: - **Area law for entanglement entropy:** The entanglement entropy between the physical sector and the sheet sector is $S_{\text{ent}} = \log N$. Using the UV scaling $N(\epsilon) \sim \epsilon^{-(d-2)}$ (Lemma 2 of the companion paper on non-injectivity), this becomes $S_{\text{ent}} = (d-2)\log(1/\epsilon)$, reproducing the Srednicki area law for entanglement entropy in quantum field theory. - **Isomorphism with holographic entanglement:** We construct an explicit linear isomorphism $\Phi$ between the sheet Hilbert space $\mathcal{H}_{\text{sheets}} = \ell^2(\mathbb{Z}_N)$ and the space of Ryu–Takayanagi minimal surfaces anchored at the boundary of region $A$. Under this isomorphism, the entanglement entropy $S_{\text{ent}} = \log N$ coincides with the holographic entanglement entropy $S_A^{\text{RT}}$ after the identification $\log N \leftrightarrow \text{Area}(\gamma_A)/(4G_N)$. This makes precise the connection between the geometric entanglement derived here and the holographic entanglement entropy of AdS/CFT. - **Lorentz invariance of entanglement entropy:** Although the sheet number $N$ depends on the observer's foliation, the entanglement entropy $S_{\text{ent}} = \log N$ is a Lorentz scalar. The topological projection operator $\hat{P}_0 = \mathbf{1}_N/N$ commutes with all Lorentz generators, and $S_{\text{ent}}$ is invariant under any change of inertial frame. This resolves the apparent tension between the observer-dependence of $N$ and the physical requirement of covariance. - **Geometric decoherence:** Quantum decoherence is the partial trace over the sheet degrees of freedom. When inter-sheet perturbations (derived from the Maxwell Topological Emergence Identity in the companion paper on electromagnetic fields) induce distinct states $|\psi_n\rangle$ on different sheets, the off-diagonal elements of the physical density matrix decay as $1/N$, producing classicality without any external environment. - **Van Raamsdonk conjecture as a theorem:** The equivalence between spacetime connectivity and quantum entanglement — conjectured by Van Raamsdonk (2010) and formalized as ER = EPR by Maldacena and Susskind (2013) — is proved as a theorem within the TPST–DGQ framework. Non-injectivity ($N > 1$), entanglement ($S_{\text{ent}} > 0$), and geometric connectivity of the $N$ spatial intersections are three equivalent statements. Removing entanglement (by measuring the sheet index) forces $N \to 1$ and disconnects the geometry, exactly as Van Raamsdonk conjectured. The paper further introduces a **Fock space structure** for variable sheet number, describing quantum fluctuations that create or destroy fold points. The associated creation and annihilation operators satisfy the bosonic algebra, identifying the fold points as quanta of a topological field. For $N = 2$, the De Giuseppe Qubit (DGQ) is the maximally entangled Bell state of the framework. The $O(1)$ gate complexity and $1/N$ decoherence suppression proved in the companion paper on the DGQ follow directly from the entanglement structure derived here. The **universal cancellation identity** $N(\epsilon) \cdot \epsilon^{d-2} = O(1)$ — alrKeywordseady shown in companion papers to regularize holographic entropy, Coulomb self-energy, the cosmological constant, and the intersection density $|\psi|^2$ — now operates at nine levels of physical theory, confirming worldline non-injectivity as the geometric engine of entanglement. This manuscript is current in Official Peer Review. 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