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Office, E.E. Quantum Entanglement. Encyclopedia. Available online: https://encyclopedia.pub/entry/58574 (accessed on 10 July 2025).
Office EE. Quantum Entanglement. Encyclopedia. Available at: https://encyclopedia.pub/entry/58574. Accessed July 10, 2025.
Office, Encyclopedia Editorial. "Quantum Entanglement" Encyclopedia, https://encyclopedia.pub/entry/58574 (accessed July 10, 2025).
Office, E.E. (2025, July 02). Quantum Entanglement. In Encyclopedia. https://encyclopedia.pub/entry/58574
Office, Encyclopedia Editorial. "Quantum Entanglement." Encyclopedia. Web. 02 July, 2025.
Quantum Entanglement
Edit

Quantum Entanglement is a fundamental physical phenomenon wherein the quantum states of two or more particles become interdependent such that the state of each particle cannot be fully described independently of the state(s) of the others—even when the particles are separated by large distances. This non-classical correlation violates the assumptions of local realism and plays a central role in the foundations of quantum mechanics, quantum information science, and emerging quantum technologies.

Quantum Entanglement Bell’s Inequalities Quantum Nonlocality EPR Paradox Quantum Teleportation Quantum Cryptography

1. Historical Background

The conceptual origins of entanglement trace back to the development of quantum mechanics in the early 20th century. In 1935, Albert Einstein, Boris Podolsky, and Nathan Rosen published their famous paper—the EPR paradox—which introduced entangled states as a thought experiment intended to demonstrate that quantum mechanics is incomplete [1]. They argued that if quantum theory were correct, it would imply “spooky action at a distance,” since measuring one particle would instantaneously affect the state of another, regardless of distance.

Shortly thereafter, Erwin Schrödinger coined the term “Verschränkung” (entanglement) to describe such non-separable quantum correlations [2]. Schrödinger recognized entanglement as “the characteristic trait of quantum mechanics,” emphasizing that it is not merely a mathematical curiosity but an essential feature distinguishing quantum systems from classical ones.

For decades, entanglement remained largely a philosophical question. It was not until the 1960s that physicist John Bell derived a set of inequalities—now known as Bell’s inequalities—which made it possible to design experiments to test the predictions of quantum mechanics against local hidden variable theories [3].

Source: NASA Science

2. Theoretical Framework

Quantum entanglement arises from the tensor product structure of Hilbert spaces in composite quantum systems [4]. Consider two particles A and B with individual quantum states represented by vectors |ψ_A⟩ and |ψ_B⟩. The general state of the combined system is a vector in the tensor product space:

∣ΨHAHB

A state is entangled if it cannot be expressed as a product of single-particle states:

|Ψ⟩ ≠ |ψ_A⟩ ⊗ |ψ_B⟩.

For example, the Bell state (or EPR pair):

is maximally entangled because no factorization into separate states exists [4]. In such a state, measuring particle A instantaneously determines the outcome of measurements on particle B, even if the two are spatially separated [4].

Entanglement is formally characterized using measures such as:

  • Von Neumann entropy of the reduced density matrix.

  • Entanglement entropy.

  • Entanglement of formation and distillable entanglement in quantum information theory.

3. Bell's Theorem and Experimental Verification

Bell's theorem, formulated in 1964, showed that no local hidden variable theory can reproduce all predictions of quantum mechanics [3]. Bell derived inequalities—such as the CHSH inequality—whose violation implies entanglement and the failure of local realism.

Experiments by Alain Aspect and colleagues in the early 1980s tested Bell inequalities using entangled photon pairs produced via parametric down-conversion [5]. Their results strongly violated Bell’s inequalities, confirming that nature exhibits non-local correlations consistent with quantum entanglement.

Subsequent experiments have closed various “loopholes,” including the detection loophole (ensuring fair sampling) and the locality loophole (ensuring spacelike separation of measurement events). In 2015, several landmark “loophole-free” Bell tests—by groups in the Netherlands, Austria, and the United States—provided compelling evidence that entanglement is a real and experimentally demonstrable phenomenon [4].

4. Entanglement in Quantum Information Science

Quantum entanglement is the cornerstone of many applications in quantum information theory and emerging quantum technologies [4]:

  • Quantum Teleportation: Entanglement enables the transfer of an unknown quantum state from one location to another, without physically transmitting the particle itself. This protocol, demonstrated experimentally in 1997, requires a shared entangled state and classical communication [6].

  • Quantum Cryptography: Entanglement-based protocols, such as Ekert's 1991 QKD scheme, exploit correlations in Bell states to detect eavesdropping [6].

  • Quantum Computing: Entanglement enables quantum parallelism and is essential for algorithms like Shor's factoring algorithm and Grover’s search algorithm. Entangled qubits form the basis of error correction codes and fault-tolerant computation [4].

  • Entanglement Swapping: This process allows two particles that have never interacted to become entangled via entanglement of intermediaries, which is crucial for quantum networks and repeater architectures [4].

5. Entanglement Entropy and Quantum Many-Body Physics

In condensed matter physics and quantum field theory, entanglement entropy has become a powerful tool to characterize correlations and phase transitions. For example:

  • In 1D critical systems described by conformal field theory, the entanglement entropy scales logarithmically with subsystem size.

  • In topologically ordered systems, entanglement entropy reveals hidden nonlocal order.

Entanglement has also provided insights into the black hole information paradox and the conjectured holographic principle, where spacetime geometry may emerge from entanglement structure [4].

6. Philosophical and Foundational Implications

Quantum entanglement challenges classical notions of separability, locality, and realism [1][2][3]:

  • Einstein's concerns about “spooky action at a distance” reflect the tension between quantum nonlocality and relativity [1].

  • Schrödinger's cat thought experiment illustrates entanglement between microscopic and macroscopic degrees of freedom, raising questions about the measurement problem [2].

  • Some interpretations of quantum mechanics—such as many-worlds and objective collapse models—propose fundamentally different resolutions to these paradoxes [4].

Entanglement remains central to debates about the completeness and interpretation of quantum theory [3].

7. Modern Developments and Experimental Progress

Recent advances include:

  • Long-distance entanglement distribution, as in the Chinese Micius satellite, which demonstrated entanglement over 1,200 km.

  • Integrated photonic circuits generating and manipulating entanglement on chip-scale devices [4].

  • Entangled ion traps and superconducting qubits, used as building blocks for scalable quantum processors [4].

  • Device-independent protocols, which rely on entanglement and Bell violations to certify randomness and security without assumptions about the internal workings of devices [4].

8. Future Directions

Research into entanglement continues to drive new frontiers:

  • Building robust quantum internet architectures.

  • Developing entanglement-enhanced metrology surpassing classical limits of measurement precision.

  • Exploring quantum gravity, where spacetime geometry itself may emerge from entanglement.

These efforts highlight that entanglement is not merely an esoteric feature of quantum theory but a transformative resource shaping 21st-century science and technology.

References

  1. Einstein, A., Podolsky, B., & Rosen, N. (1935). Can Quantum-Mechanical Description of Physical Reality Be Considered Complete? Physical Review, 47(10), 777–780. https://doi.org/10.1103/PhysRev.47.777
  2. Schrödinger, E. (1935). Discussion of Probability Relations between Separated Systems. Mathematical Proceedings of the Cambridge Philosophical Society, 31(4), 555–563. https://doi.org/10.1017/S0305004100013554
  3. Bell, J. S. (1964). On the Einstein Podolsky Rosen Paradox. Physics Physique Физика, 1(3), 195–200. https://doi.org/10.1103/PhysicsPhysiqueFizika.1.195.
  4. Aspect, A., Dalibard, J., & Roger, G. (1982). Experimental Test of Bell’s Inequalities Using Time-Varying Analyzers. Physical Review Letters, 49(25), 1804–1807. https://doi.org/10.1103/PhysRevLett.49.1804.
  5. Aspect, A., Dalibard, J., & Roger, G. (1982). Experimental Test of Bell’s Inequalities Using Time-Varying Analyzers. Physical Review Letters, 49(25), 1804–1807. https://doi.org/10.1103/PhysRevLett.49.1804.
  6. Bennett, C. H., Brassard, G., Crépeau, C., Jozsa, R., Peres, A., & Wootters, W. K. (1993). Teleporting an Unknown Quantum State via Dual Classical and Einstein-Podolsky-Rosen Channels. Physical Review Letters, 70(13), 1895–1899. https://doi.org/10.1103/PhysRevLett.70.1895.
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