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Bound entanglement

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than separable states. Families of bound entangled states known analytically even for high dimension that outperform separable states for metrology. For large dimensions they approach asymptotically the maximal precision achievable by bipartite quantum states. There are bipartite bound entangled
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While no singlets can be distilled from bound entangled state, they can be still useful for some quantum information processing applications. Bound entanglement can be activated. Any entangled state can enhance the teleportation power of some other state. This holds even if the state is bound
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It has been shown that bipartite bound entangled states with a positive partial transpose exist in symmetric systems. It has also been shown that in symmetric systems multipartite bound entangled states exists for which all partial transposes are non-negative.
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There are also multipartite entangled states that have a negative partial transpose with respect to some bipartitions, while they have a positive partial transpose to the other partitions, nevertheless, they are undistillable.
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conjectured that bipartite bound entangled states with positive partial transpose cannot violate a Bell inequality. After a long search for counterexamples, the conjecture turned out to be false.
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DiVincenzo, David P.; Shor, Peter W.; Smolin, John A.; Terhal, Barbara M.; Thapliyal, Ashish V. (17 May 2000). "Evidence for bound entangled states with negative partial transpose".
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Tura, J.; Augusiak, R.; Hyllus, P.; KuĹ›, M.; Samsonowicz, J.; Lewenstein, M. (22 June 2012). "Four-qubit entangled symmetric states with positive partial transpositions".
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Piani, Marco; Mora, Caterina E. (4 January 2007). "Class of positive-partial-transpose bound entangled states associated with almost any set of pure entangled states".
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states that are not more useful than separable states, but if an auxiliary qubit is added to one of the subsystems then they outperform separable states in metrology.
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Bipartite bound entangled states with a positive partial transpose are useless for teleportation, as they cannot lead to a larger fidelity than the classical limit.
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Horodecki, Michał; Horodecki, Paweł; Horodecki, Ryszard (15 June 1998). "Mixed-State Entanglement and Distillation: Is there a "Bound" Entanglement in Nature?".
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Horodecki, Michał; Horodecki, Paweł; Horodecki, Ryszard (1 September 1999). "General teleportation channel, singlet fraction, and quasidistillation".
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Horodecki, Pawel; Smolin, John A; Terhal, Barbara M; Thapliyal, Ashish V (January 2003). "Rank two bipartite bound entangled states do not exist".
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are all bound-entangled. Moreover, a particular quantum state for 2x4 systems has been presented. Such states are not detected by the
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as entangled, thus other entanglement criteria are needed for their detection. There are a number of examples for such states.
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Chen, Lin; Tang, Wai-Shing (2 February 2017). "Schmidt number of bipartite and multipartite states under local projections".
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The possible existence of bipartite bound entangled states with a negative partial transpose is still under intensive study.
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Bennett, Charles H.; DiVincenzo, David P.; Mor, Tal; Shor, Peter W.; Smolin, John A.; Terhal, Barbara M. (28 June 1999).
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Horodecki, Paweł; Horodecki, Michał; Horodecki, Ryszard (1 February 1999). "Bound Entanglement Can Be Activated".
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Masanes, LluĂ­s (17 April 2006). "All Bipartite Entangled States Are Useful for Information Processing".
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BruĂź, Dagmar; Peres, Asher (4 February 2000). "Construction of quantum states with bound entanglement".
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entangled. Bipartite entangled states with a non-negative partial transpose can be more useful for
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Breuer, Heinz-Peter (22 August 2006). "Optimal Entanglement Criterion for Mixed Quantum States".
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Bound entangled states with a positive partial transpose in 3x3 systems have a Schmidt number 2.
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Bipartite bound entangled states do not exist in 2x2 or 2x3 systems, only in larger ones.
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TĂłth, GĂ©za; GĂĽhne, Otfried (1 May 2009). "Entanglement and Permutational Symmetry".
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Smolin, John A. (9 February 2001). "Four-party unlockable bound entangled state".
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Tóth, Géza; Vértesi, Tamás; Horodecki, Paweł; Horodecki, Ryszard (7 July 2020).
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Pál, Károly F.; Tóth, Géza; Bene, Erika; Vértesi, Tamás (10 May 2021).
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Properties of bound entangled states with a positive partial transpose
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with local operations and classical communication (
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Horodecki 36: 19: 18: 815:(1): 5297. 89:Asher Peres 1121:1911.02592 1070:2002.12409 1003:1709.03995 616:1609.05100 609:(75): 75. 104:References 1038:206306250 910:119390324 822:1405.4502 755:118386611 730:1203.3711 669:0812.4453 588:119532807 437:119474939 157:111379972 28:distilled 1162:Category 1148:32701319 1030:29376687 971:10914899 963:16712136 849:25370352 702:43527866 694:19518768 641:34893860 535:43737866 490:37213011 384:55900164 331:14406014 323:17026285 270:14688979 1126:Bibcode 1075:Bibcode 1008:Bibcode 943:Bibcode 890:Bibcode 857:5135148 827:Bibcode 790:9697993 735:Bibcode 674:Bibcode 621:Bibcode 568:Bibcode 470:Bibcode 417:Bibcode 364:Bibcode 303:Bibcode 250:Bibcode 210:7019402 190:Bibcode 137:Bibcode 1146:  1036:  1028:  969:  961:  908:  855:  847:  788:  753:  700:  692:  639:  586:  533:  488:  435:  382:  329:  321:  268:  208:  155:  45:, and 1116:arXiv 1065:arXiv 1034:S2CID 998:arXiv 967:S2CID 933:arXiv 906:S2CID 880:arXiv 853:S2CID 817:arXiv 786:S2CID 751:S2CID 725:arXiv 698:S2CID 664:arXiv 637:S2CID 611:arXiv 584:S2CID 558:arXiv 531:S2CID 513:arXiv 486:S2CID 460:arXiv 433:S2CID 407:arXiv 380:S2CID 354:arXiv 327:S2CID 293:arXiv 266:S2CID 240:arXiv 228:(PDF) 206:S2CID 180:arXiv 153:S2CID 127:arXiv 1144:PMID 1026:PMID 959:PMID 845:PMID 690:PMID 319:PMID 34:). 32:LOCC 1134:doi 1112:125 1083:doi 1016:doi 994:120 951:doi 898:doi 835:doi 778:doi 743:doi 682:doi 660:102 629:doi 576:doi 523:doi 509:292 478:doi 425:doi 372:doi 311:doi 258:doi 198:doi 145:doi 1164:: 1142:. 1132:. 1124:. 1110:. 1106:. 1081:. 1073:. 1059:. 1055:. 1032:. 1024:. 1014:. 1006:. 992:. 988:. 965:. 957:. 949:. 941:. 929:96 927:. 904:. 896:. 888:. 876:82 874:. 851:. 843:. 833:. 825:. 811:. 807:. 784:. 774:29 772:. 749:. 741:. 733:. 721:85 719:. 696:. 688:. 680:. 672:. 658:. 635:. 627:. 619:. 607:16 605:. 582:. 574:. 566:. 554:60 552:. 529:. 521:. 507:. 484:. 476:. 468:. 456:61 454:. 431:. 423:. 415:. 403:63 401:. 378:. 370:. 362:. 350:75 348:. 325:. 317:. 309:. 301:. 289:97 287:. 264:. 256:. 248:. 236:82 234:. 230:. 204:. 196:. 188:. 176:61 174:. 151:. 143:. 135:. 123:80 121:. 41:, 1150:. 1136:: 1128:: 1118:: 1091:. 1085:: 1077:: 1067:: 1061:3 1040:. 1018:: 1010:: 1000:: 973:. 953:: 945:: 935:: 912:. 900:: 892:: 882:: 859:. 837:: 829:: 819:: 813:5 792:. 780:: 757:. 745:: 737:: 727:: 704:. 684:: 676:: 666:: 643:. 631:: 623:: 613:: 590:. 578:: 570:: 560:: 537:. 525:: 515:: 492:. 480:: 472:: 462:: 439:. 427:: 419:: 409:: 386:. 374:: 366:: 356:: 333:. 313:: 305:: 295:: 272:. 260:: 252:: 242:: 212:. 200:: 192:: 182:: 159:. 147:: 139:: 129::

Index

quantum entanglement
distilled
LOCC
M. Horodecki
P. Horodecki
R. Horodecki
partial transpose
Peres-Horodecki criterion
Asher Peres
quantum metrology
arXiv
quant-ph/9801069
Bibcode
1998PhRvL..80.5239H
doi
10.1103/PhysRevLett.80.5239
S2CID
111379972
arXiv
quant-ph/9911056
Bibcode
2000PhRvA..61c0301B
doi
10.1103/PhysRevA.61.030301
S2CID
7019402
"Unextendible Product Bases and Bound Entanglement"
arXiv
quant-ph/9808030
Bibcode

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