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Quantum Entanglement


Quantum entanglement is the failure of a joint quantum state to be expressible as a convex combination of product states. For finite-dimensional Hilbert spaces A and B, a density matrix rho is separable when it can be written

 rho=sum_(i)p_irho_i^A tensor rho_i^B,

with p_i>=0, sum_(i)p_i=1, and density matrices rho_i^A and rho_i^B. A state that is not separable is entangled. A pure state is separable precisely when its defining unit vector is a tensor product.

For example, (|00>+|11>)/sqrt(2) is an entangled pure state of two quantum bits. The unentanglement promise in QMA(2) and the approximation problem in the no-disentanglers conjecture depend on this distinction between separable states and arbitrary joint states.


See also

Density Matrix, Hilbert Space, No-Disentanglers Conjecture, QMA, Quantum Bit, Tensor Product

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References

Bostanci, J.; Grewal, S.; Haferkamp, J.; Huang, A.; Hwang, Y.; Natarajan, A.; and Nirkhe, C. "A Quantum Oracle Separation Between QMA(2) and QMA." 2 Sep 2026. https://arxiv.org/abs/2609.02865.Watrous, J. The Theory of Quantum Information. Cambridge, England: Cambridge University Press, 2018. https://doi.org/10.1017/9781316848142.

Cite this as:

Weisstein, Eric W. "Quantum Entanglement." From MathWorld--A Wolfram Resource. https://mathworld.wolfram.com/QuantumEntanglement.html

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