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This article is reprinted in J. Wheeler and W. Zureck, Quantum Measurement Theory (Princeton University Press, Princeton, 1983).
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The concept of entanglement swapping was first introduced by PRLTAO 0031-9007 10.1103/PhysRevLett.71.4287
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The concept of entanglement swapping was first introduced by M. Zukowski, A. Zeilinger, M. A. Horne, and A. K. Ekert, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.71.4287 71, 4287 (1993).
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For a discussion of the low detection efficiency, random sampling, and other loopholes, see, for example, Clarendon, Oxford
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For a discussion of the low detection efficiency, random sampling, and other loopholes, see, for example, M. Redhead, Incompleteness, Nonlocality, and Realism (Clarendon, Oxford, 1987);
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The first two-particle proof, which held for only about 16% of all cases, was given by PRLTAO 0031-9007 10.1103/PhysRevLett.71.1665
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The first two-particle proof, which held for only about 16% of all cases, was given by L. Hardy, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett. 71.1665 71, 1665 (1993).
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The first complete proof for the case of two-particles and four observers was given by PRLTAO 0031-9007 10.1103/PhysRevLett.86.1911
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The first complete proof for the case of two-particles and four observers was given by A. Cabello, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett. 86.1911 86, 1911 (2001).
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Many of the results of papers [8-14] were previously arrived at by PRLTAO 0031-9007 10.1103/PhysRevLett.73.3191
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Many of the results of papers [8-14] were previously arrived at by M. Pavicic and J. Summhammer, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.73.3191 73, 3191 (1994);
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