Quantum entanglement is traditionally framed as spatial non-locality: two particles at arbitrary separation maintain correlated states, with measurement of one instantaneously affecting the other. We propose a reformulation: entanglement is fundamentally a temporal phenomenon — a synchronization of quantum phases via universal harmonic oscillations. Spatial entanglement is recovered as the special case where both particles are created at the same time and location. Three independent experiments support this framework: (1) Megidish et al. (2013) demonstrated entanglement between photons that never coexisted; (2) temporal qubit encoding (|𝜓⟩ = 𝛼|early⟩ + 𝛽|late⟩) achieves full quantum information capacity; (3) Jiang et al. (2024) measured entanglement formation taking 232 attoseconds — the time for a wave to establish phase coherence. In the Fractal Mechanics framework, all particles oscillate at Fibonacci-harmonic frequencies 𝜔_𝑛 = 𝜔_𝑃×(𝜑^−𝑛), and entanglement is their synchronization to common harmonics. This formulation predicts that entanglement fidelity is maximized for time separations Δ𝑡_𝑛 = 𝑇₀/𝜑^𝑛 (Fibonacci timing), testable with current attosecond technology.
Quantum entanglement is traditionally framed as spatial non-locality: two particles at arbitrary separation maintain correlated states, with measurement of one instantaneously affecting the other. We propose a reformulation: entanglement is fundamentally a temporal phenomenon — a synchronization of quantum phases via universal harmonic oscillations. Spatial entanglement is recovered as the special case where both particles are created at the same time and location. Three independent experiments support this framework: (1) Megidish et al. (2013) demonstrated entanglement between photons that never coexisted; (2) temporal qubit encoding (|𝜓⟩ = 𝛼|early⟩ + 𝛽|late⟩) achieves full quantum information capacity; (3) Jiang et al. (2024) measured entanglement formation taking 232 attoseconds — the time for a wave to establish phase coherence. In the Fractal Mechanics framework, all particles oscillate at Fibonacci-harmonic frequencies 𝜔_𝑛 = 𝜔_𝑃×(𝜑^−𝑛), and entanglement is their synchronization to common harmonics. This formulation predicts that entanglement fidelity is maximized for time separations Δ𝑡_𝑛 = 𝑇₀/𝜑^𝑛 (Fibonacci timing), testable with current attosecond technology.
Quantum entanglement presents a fundamental challenge to relativistic causality, as measurements on one particle instantaneously affect its entangled partner regard- less of spatial separation. We propose a complete theoretical framework—Dynamical Scalar Field Theory (DSFT)—in which entanglement is not a nonlocal correlation but a topological remnant of the pre-Big Bang Euclidean phase. In this framework, two entangled particles reside at a single point in the scalar field configuration space, connected by a static topological soliton (phase-locking filament) where the classi- cal time dimension remains frozen (Ω = 0). We derive the full Lagrangian from first principles, including non-minimal coupling to matter and curvature, and demon- strate that the decoherence process corresponds to a sudden geometric phase tran- sition (Ω : 0 → 1) occurring within ∆tjump = 85.2 ± 0.4 attoseconds—independent of spatial distance. Our numerical simulations yield precise predictions: a thermal pulse of power Pthermal = 2.36 × 10−4 W, an entropy jump ∆S = 1.46 × 10−22 J/K, and a high-frequency gravitational wave signature at f ∼ 106 Hz with strain ampli- tude h ∼ 10−38. These predictions align quantitatively with unexplained noise in superconducting qubits (IBM/Google) and attosecond time delays in photoionization experiments (Max Planck 2024). We propose a definitive experimental protocol us- ing Ramsey interferometry and TES bolometry to test the distance-independence of the decoherence time—a unique and falsifiable prediction of DSFT. This work estab- lishes entanglement as a manifestation of un-crystallized spacetime geometry, resolvable through attosecond and quantum thermodynamics experiments
Abstract Quantum entanglement is the most famous nonlocal phenomenon in modern physics, and its instantaneous ultra-distance correlation has puzzled physicists for nearly a century. Einstein referred to this effect as “spooky action at a distance”, because it seemingly violates the local causality and light-speed limit of general relativity. Traditional physical theories can only describe entanglement through mathematical wave functions but cannot explain its fundamental physical origin. Based on the three-dimensional time quantization unified field theory, this paper proposes a novel physical mechanism for quantum entanglement. The instantaneous synchronization of entangled particles does not rely on spatial signal transmission, but originates from the shared coupling of the fluctuating time dimension. Quantum systems can bypass classical spatial restrictions through time-dimensional resonance, perfectly explaining quantum nonlocality without violating relativistic rules. This study fundamentally resolves the core contradiction between quantum mechanics and general relativity, reveals the essential nature of entanglement, and completes the systematic theoretical verification of the three-dimensional time unified field framework. AI Usage Note: All theoretical ideas, mathematical derivations and conclusions are independently created by the author. Generative AI was only used for linguistic polishing of sentences. The author takes full responsibility for all content.
Quantum entanglement—the instantaneous correlation of measurements on spatially separated particles—has been described as 'spooky action at a distance.' This paper proposes that entanglement requires no action and involves no distance: entangled particles are nodes on the same standing wave. We prove four theorems establishing the mathematical equivalence: (1) standing wave nodes are correlated by identity, not communication; (2) phase coherence requires identical frequency; (3) quantum phase equals wave phase; (4) entangled particles are phase-locked by conservation laws. This interpretation explains why entanglement is instantaneous (no signal travels—the wave is already correlated everywhere), why no information can be transmitted (measurement outcomes are random), and why entanglement is fragile (any frequency perturbation breaks coherence). The standing wave interpretation is compatible with Bell's theorem because standing waves are nonlocal by definition—Bell forbids only local hidden variables. We propose testable predictions including correlation between entanglement fidelity and frequency precision, and the possibility of 'harmonic entanglement' between particles at resonant frequency ratios.
Erwin Schrodinger first used the phrase “quantum entanglement” in 1935 to describe a mechanical phenomenon at the quantum level where two (or more) particles’ quantum states must be defined in relation to one another even if they may be geographically apart. This paradoxical event has confounded us for a very long time. Entangled particle behavior appears to be mysterious, illogical, and akin to sorcery at work. The successful and dependable principle of locality has led us to the achievements of twentieth-century physics. However, some theorists may doubt the locality itself due to the “spooky” and nonlocal effects of the local laws of quantum theory. Could there truly be an instant connection between two subatomic particles located on the extreme edges of the universe? Is there a theory that predicts such a relationship that is fundamentally faulty or lacking? Are the outcomes of the experiments that show this connection being read incorrectly? These questions challenge our most fundamental understanding of space and time. The universe is currently being disassembled by modern physics, and it will never be the same. Utilizing cutting-edge technology, quantum entanglement will have a positive impact on society. The history of quantum entanglement is outlined in this work, along with several hypotheses regarding the puzzling behavior of entangled particles. Quantum entanglement may also be an instance of nonlocality in action, in which what occurs in one location affects what occurs in another. Entanglement can also be compared to a situation in which a light switch is used to control two (or more) light bulbs, causing them to turn on at the same time when the switch is switched on. The key question is whether one of the aforementioned theories actually accounts for the odd behavior of entangled particles, in which case experimental evidence would unquestionably support the theory.
The theory of Quantum Mechanics is one of the mainstay of modern physics, a well-established mathematical clockwork whose strength and accuracy in predictions are currently experienced in worldwide research laboratories. As a matter of fact, Quantum Mechanics laid the groundwork of a rich variety of studies ranging from solid state physics to cosmology, from bio-physics to particle physics. The up-to-date ability of manipulating single quantum states is paving the way for emergent quantum technologies as quantum information and computation, quantum communication, quantum metrology and quantum imaging. In spite of the impressive matemathical capacity, a long-standing debate is even revolving around the foundational axioms of this theory, the main bones of content being the non-local effects of entangled states, the wave function collapse and the concept of measurement in Quantum Mechanics, the macro-objectivation problem (the transition from a microscopic probabilistic world to a macroscopic deterministic world described by classical mechanics). Problems that, beyond their fundamental interest in basic science, now also concern the impact of these developing technologies. Without claiming to be complete, this article provides in outline the living matter concerning some of these problems, the implications of which extend deeply on the connection between entanglement and space-time structure.
Entanglement in the S-Field 1. Ontic basis of entanglement In the S-framework, each particle is a two-mode S-oscillator: Φ = (Φ_sb , Φ_bs). Entanglement occurs when two or more S-oscillators share a common S-phase structure. This is not information transmission between particles in B-space — it is a single, joint S-configuration projected into multiple B-locations. Thus entanglement is a multi-projection of one S-state, not a correlation between two separ ate B-states. 2. Shared S-Phase Condition (the core definition) Let particles A and B have states: Φ_A = (A_sb exp(i φ_A_sb), A_bs exp(i φ_A_bs)) Φ_B = (B_sb exp(i φ_B_sb), B_bs exp(i φ_B_bs)). They are entangled if and only if: Δφ_A = Δφ_B, and the bs-components satisfy a joint coherence: Φ_A_bs = λ Φ_B_bs, where λ is a complex ratio with |λ| fixed during the entangled interval. This means: The S-components form a single connected oscillatory object. Mathematically, define the Joint S-State: Ψ_S = Φ_A_bs ⊗ Φ_B_bs. Entanglement corresponds to: rank(Ψ_S) = 1. This is the most compact mathematical expression of entanglement in this theory. 3. Why entanglement is instantaneous Inside the S-domain: • there is no spatial metric • there is no propagation • there is only phase structure. Thus a change in Φ_A_sb or Φ_A_bs that forces a new Δφ_A immediately alters Δφ_B because both projections originate from the same Ψ_S. This explains experimental observations: • zero-time correlations • infinite effective signaling speed • independence from spatial separation • no energy or momentum transfer. All of them follow automatically from: S has no distance and no finite propagation speed. 4. Collapse as B-projection selection Measurement is interpreted as: P_B Φ_A → specific eigen-projection. Because A and B share the same Ψ_S, selecting one B-projection forces the entire Ψ_S to project consistently. Thus: Measurement collapse is not a physical signal. It is selection of one branch of a shared S-object. No superluminal influence is needed. 5. Conservation laws Because both particles share the same S-state: • Spin correlations • Momentum conservation • Polarization complements appear automatically from the structure of Ψ_S: Ψ_S = Φ_A_bs ⊗ Φ_B_bs. Constraints on Φ_A_bs impose the complementary constraints on Φ_B_bs. Thus conservation laws are not maintained through 3D interaction, but through S-symmetry of the joint state. 6. Entanglement swapping and teleportation Teleportation in the S-framework is simple: 1. Two particles share Ψ_S₁. 2. One particle from Ψ_S₁ interacts with a particle from Ψ_S₂. 3. Their S-phases align (Δφ matching). 4. This merges Ψ_S₁ and Ψ_S₂ into a new unified Ψ_S. The B-space interpretation is “entanglement swapping,” but the S-interpretation is: merging or re-partitioning of phase-coherent S-objects. Teleportation = transfer of B-state through S-resonance alignment, not physical movement. 7. Unified S-Equation of Entanglement The full formal criterion for entanglement is: P_S (Φ_A ⊗ Φ_B) ≠ (P_S Φ_A) ⊗ (P_S Φ_B). This inequality means: “The S-projection of the joint system cannot be expressed as a product of the S-projections of its parts.” Or verbally: Entanglement is non-factorability of the S-projection. This matches all known experimental results but gives a far clearer ontology. Summary in one sentence Entanglement is the multi-location projection of a single S-phase coherent structure into baryonic space, explaining the instantaneous correlations and nonlocal behavior naturally.