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Quantum entanglement
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=== Methods of creating entanglement === Entanglement is usually created by direct interactions between subatomic particles. These interactions can take numerous forms. One of the most commonly used methods is [[spontaneous parametric down-conversion]] to generate a pair of photons entangled in polarization.<ref name="horodecki2007"> {{cite journal |last1 = Horodecki |first1 = Ryszard |last2 = Horodecki |first2 = Pawel |last3 = Horodecki |first3 = Michal |last4 = Horodecki |first4 = Karol |title = Quantum entanglement |journal = Reviews of Modern Physics |arxiv=quant-ph/0702225 |doi =10.1103/RevModPhys.81.865 |year=2009 |pages=865โ942 |bibcode=2009RvMP...81..865H |volume=81 |issue=2 |s2cid=59577352 }}</ref><ref name="Shadbolt2012"> {{cite journal |last1=Shadbolt |first1=P. J. |last2=Verde |first2=M. R. |last3=Peruzzo |first3=A. |last4=Politi |first4=A. |last5=Laing |first5=A. |last6=Lobino |first6=M. |last7=Matthews |first7=J. C. F. |last8=Thompson |first8=M. G. |last9=O'Brien |first9=J. L. |title=Generating, manipulating and measuring entanglement and mixture with a reconfigurable photonic circuit |journal=Nature Photonics |year=2012 |volume=6 |issue=1 |pages=45โ59 |arxiv=1108.3309 |doi=10.1038/nphoton.2011.283 |bibcode = 2012NaPho...6...45S |s2cid=56206588 }}</ref> Other methods include the use of a [[fibre coupler]] to confine and mix photons, photons emitted from decay cascade of the bi-exciton in a [[quantum dot]],<ref>{{cite journal |last=Akopian |first=N. |date=2006 |title=Entangled Photon Pairs from Semiconductor Quantum Dots |journal=Physical Review Letters |volume=96 |issue=2 |pages=130501 |arxiv=quant-ph/0509060 |bibcode=2006PhRvL..96b0501D |doi=10.1103/PhysRevLett.96.020501 |pmid=16486553 |s2cid=22040546 }}</ref> or the use of the [[HongโOuโMandel effect]].<ref>{{cite journal|last1=Lee |first1=Hwang |last2=Kok |first2=Pieter |last3=Dowling |first3=Jonathan P. |author-link3=Jonathan Dowling |title=A quantum Rosetta stone for interferometry |journal=Journal of Modern Optics |volume=49 |number=14โ15 |year=2002 |pages=2325โ2338 |doi=10.1080/0950034021000011536 |arxiv=quant-ph/0202133|bibcode=2002JMOp...49.2325L}}</ref> Quantum entanglement of a [[elementary particle|particle]] and its [[antiparticle]], such as an electron and a [[positron]], can be created by partial overlap of the corresponding [[quantum wave function]]s in [[Hardy's paradox|Hardy's interferometer]].<ref name="Hardy1992"> {{cite journal | last = Hardy | first = Lucien | title = Quantum mechanics, local realistic theories, and Lorentz-invariant realistic theories | journal = Physical Review Letters | volume = 68 | number = 20 | pages = 2981โ2984 | doi = 10.1103/PhysRevLett.68.2981 | year = 1992 | pmid = 10045577 | bibcode = 1992PhRvL..68.2981H }}</ref><ref name="Georgiev2022"> {{cite journal | last1 = Georgiev | first1 = Danko | last2 = Cohen | first2 = Eliahu | title = Entanglement measures for two-particle quantum histories | journal = Physical Review A | volume = 106 | number = 6 | pages = 062437 | doi = 10.1103/PhysRevA.106.062437 | arxiv = 2212.07502 | year = 2022 | bibcode = 2022PhRvA.106f2437G | s2cid = 254685902 }}</ref> In the earliest tests of Bell's theorem, the entangled particles were generated using [[atomic cascade]]s.<ref name="Clauser"/> It is also possible to create entanglement between quantum systems that never directly interacted, through the use of [[Quantum teleportation#Entanglement swapping|entanglement swapping]]. Two independently prepared, identical particles may also be entangled if their wave functions merely spatially overlap, at least partially.<ref>{{cite journal |last1=Lo Franco |first1=Rosario |last2=Compagno |first2=Giuseppe |date=14 June 2018 |title=Indistinguishability of Elementary Systems as a Resource for Quantum Information Processing |journal=Physical Review Letters |volume=120 |issue=24 |pages=240403 |arxiv=1712.00706 |bibcode=2018PhRvL.120x0403L |doi=10.1103/PhysRevLett.120.240403 |pmid=29957003 |s2cid=49562954}}</ref>
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