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84868942235
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MSSM (defined in Eq. 1) contain one full ebit of entanglement as described in more detail in (19).
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MSSM (defined in Eq. 1) contain one full ebit of entanglement as described in more detail in (19).
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The second approach of (24), based on distillation, does not immediately generalize from their pure states to our mixed states: Under the constraint of single-qubit operations one cannot produce-with unit probability-n-party [Greenberger-Horne-Zeilinger] states for n > 1.
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The second approach of (24), based on distillation, does not immediately generalize from their pure states to our mixed states: Under the constraint of single-qubit operations one cannot "produce-with unit probability-n-party [Greenberger-Horne-Zeilinger] states" for n > 1.
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84868942236
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We thank P. Kok for helpful discussions. This research is supported by the Engineering and Physical Sciences Research Council through the Quantum Information Processing Interdisciplinary Research Collaboration, GR/S82176/01) and CAESR (EP/D048559/1, J.F. is supported by Merton College, Oxford. G.A.D.B. is supported by the EPSRC GR/S15808/01, J.J.L.M. acknowledges St. John's College, Oxford. J.J.L.M, S.C.B, and A.A. acknowledge support from the Royal Society
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We thank P. Kok for helpful discussions. This research is supported by the Engineering and Physical Sciences Research Council through the Quantum Information Processing Interdisciplinary Research Collaboration (www.qipirc.org) (GR/S82176/01) and CAESR (EP/D048559/1). J.F. is supported by Merton College, Oxford. G.A.D.B. is supported by the EPSRC (GR/S15808/01). J.J.L.M. acknowledges St. John's College, Oxford. J.J.L.M., S.C.B., and A.A. acknowledge support from the Royal Society.
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