Quantum entanglement is a physical phenomenon that occurs when a group of particles is generated, interact, or share spatial proximity in a way such that the quantum state of each particle of the group cannot be described independently of the state of the others, including when the particles are separated by a large distance.[1] The measurement of a quantum property of one entangled particle is correlated with the measurement of the same property in another.[2]
Albert Einstein famously referred to entanglement as "spooky action at a distance" due to its counterintuitive nature and the apparent violation of local realism.[3] However, modern physics has established entanglement as a fundamental resource in quantum information science, forming the basis for quantum computing, quantum cryptography, and quantum teleportation.
Historical Background
The phenomenon was first systematically discussed in the 1935 Einstein-Podolsky-Rosen (EPR) paradox paper, which aimed to demonstrate that quantum mechanics was an incomplete description of physical reality.[4] The authors argued that if quantum mechanics were complete, it would imply non-local influences contradicting the principle of locality.
In 1935, Erwin Schrödinger published a follow-up paper coining the term "Verschränkung" (entanglement), calling it "the characteristic trait of quantum mechanics."[5] For decades, entanglement remained a philosophical debate until John Stewart Bell formulated his famous theorem in 1964, providing a testable mathematical framework to distinguish between local hidden variable theories and quantum mechanics.
Mathematical Formulation
In quantum mechanics, entanglement arises from the tensor product structure of composite systems. A bipartite pure state |ψ⟩ in the Hilbert space HA ⊗ HB is entangled if it cannot be written as a product state |ψA⟩ ⊗ |ψB⟩.[6]
Bell Inequalities
Bell's theorem demonstrates that no local hidden variable theory can reproduce all predictions of quantum mechanics. The CHSH inequality provides a practical experimental test:
S(AB) = |E(a,b) - E(a,b') + E(a',b) + E(a',b')| ≤ 2
Quantum mechanics predicts a maximum value of 2√2 ≈ 2.828, violating the classical bound and confirming the non-local nature of entanglement.[7]
Density Matrices
For mixed states, entanglement is characterized by the reduced density matrix. A state ρAB is separable if it can be written as a convex combination of product states: ρAB = Σi pi ρA(i) ⊗ ρB(i). States that cannot be decomposed this way are entangled.[8]
Experimental Verification
Experimental tests of Bell inequalities began in the 1970s and improved significantly through the 1980s and 1990s. Alain Aspect's 1982 experiments closed the locality loophole by rapidly switching measurement settings during photon flight.[9] Subsequent experiments by Zeilinger, Clauser, and others addressed detection and freedom-of-choice loopholes, culminating in loophole-free Bell tests in 2015.[10]
The 2022 Nobel Prize in Physics was awarded to Alain Aspect, John F. Clauser, and Anton Zeilinger "for experiments with entangled photons, establishing the violation of Bell inequalities and pioneering quantum information science."[11]
Applications
Entanglement is not merely a theoretical curiosity but a practical resource driving the second quantum revolution.
Quantum Teleportation
Quantum teleportation allows the transfer of an unknown quantum state from one location to another using entanglement and classical communication. First demonstrated in 1997, it has since been achieved over hundreds of kilometers via satellite links.[12]
Quantum Cryptography
Entanglement-based quantum key distribution (QKD), such as the E91 protocol, provides theoretically unconditional security based on the laws of physics rather than computational complexity.[13] Any eavesdropping attempt inevitably disturbs the entangled states, revealing the presence of an intruder.
See Also
References
- Nielsen, M. A., & Chuang, I. L. (2010). Quantum Computation and Quantum Information. Cambridge University Press. p. 43.
- Shimony, A. (1995). "Comment on 'Quantum Entanglement'". Physics Today, 48(4), 23.
- Einstein, A. (1949). "Discussion on the General Conceptual Basis of Quantum Mechanics". In Schilpp, P. A. (Ed.), Albert Einstein: Philosopher-Scientist. Harper & Brothers. p. 68.
- Einstein, A., Podolsky, B., & Rosen, N. (1935). "Can Quantum-Mechanical Description of Physical Reality Be Considered Complete?". Physical Review, 47(10), 777–780.
- Schrödinger, E. (1935). "Die gegenwärtige Situation in der Quantenmechanik". Naturwissenschaften, 23(49), 807–812.
- Walter, M., & Kraskov, A. (2019). "Measuring Entanglement via Local Computations". Journal of Physics A, 52(39), 393001.
- Clauser, J. F., & Horne, M. A. (1974). "Experimental consequences of objective local theories". Physical Review D, 10(12), 526–535.
- Werner, R. F. (1989). "Quantum states with Einstein-Podolsky-Rosen correlations admitting a hidden-variable model". Physical Review A, 40(8), 4277.
- Aspect, A., Grangier, P., & Roger, G. (1982). "Experimental Realization of Einstein-Podolsky-Rosen-Bohm Gedankenexperiment". Physical Review Letters, 49(2), 91–94.
- Hensen, B., et al. (2015). "Loophole-free Bell inequality violation using electron spins separated by 1.3 kilometres". Nature, 526(7575), 682–686.
- The Nobel Prize in Physics 2022. Royal Swedish Academy of Sciences. Retrieved from nobelprize.org
- Bouwmeester, D., et al. (1997). "Experimental Quantum Teleportation". Nature, 390(6660), 575–579.
- Ekert, A. K. (1991). "Quantum Cryptography Based on Bell's Theorem". Physical Review Letters, 67(6), 661–663.