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diff of Teleportation

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v3:2004-05-04 09:56:18(6,516), v4:2004-05-04 10:05:28(6,795)
diff v3:jiinny v4:jiinny

= \def@alink=Articles:teleportation/%s
=
= \@ocat
= \@hcat{Research}
= \@hcat{ArticlesCategory}
= \@cat{BibliographicCategory}
= \@ecat
= #[Barnett-Phoenix 91] (¡°index of correlation¡±), \n
= # [Bennett-Brassard-Crepeau-(+3) 93],
= # [Sud-bery 93] (News and views, Nature),
= # [Deutsch-Ekert 93],
- # [Popescu 94],
- # [Vaidman 94 a],
+ # [Popescu 94|\@alink{(94 Popesu) Bells Inequalities versus Teleportatin- What is Nonlocality-PRL_v72_p797.pdf}],
+ # [Vaidman 94 a|\@alink{(94a Vaidman)Teleportation of quantum states-PRA_v49_p1473.pdf}],
= # [Davidovich-Zagury-Brune-(+2) 94|\@alink{(94 Davidovich-Zagury-Brune-(+2))Teleportation of anatomic state between two cavities using nonlocal microwave fields_PRA_v50_pR895.pdf}],
= # [Cirac-Parkins 94|\@alink{(94 Cirac-Parkins)Schemes for atomic-state teleportation_PRA_v50_pR4441.pdf}],
= # [Braunstein-Mann 95],
- # [Vaidman 95 c],
+ # [Vaidman 95 c|\@alink{(95c Vaidman)Bells Inequalities and Density Matrices-Revealing Hidden Nonlocality-PRL_v74_p2619.pdf}],
= # [Popescu 95],
= # [Gisin 96 b],
= # [Bennett-Brassard-Popescu-(+3) 96],
= # [Horodecki-Horodecki-Horodecki 96 b],
= # [Horodecki-Horodecki 96 b|\@alink{(96 Horodecki-Horodecki) Information-theoretic aspects of inseparability of mixed states PRA_v54_p1838.pdf}] - <i>cf</i>. [Horodecki-Horodecki-Horodecki 96 a|\@alink{(96 Horodecki-Horodecki-Horodeki)Quantum alpha-entropy inequalities-independent condition for local realism.pdf}]
= # [Taubes 96],
= # [Braunstein 96 a],
= # [Home 97] (Sec. 4. 4),
= # [Moussa 97 a],
= # [Nielsen-Caves 97] (reversible quantum operations and their application to T),
= # [Zheng-Guo 97 a, b],
= # [Watson 97 b],
= # [Anonymous 97],
= # [Williams-Clearwater 98] (book with a chapter on T),
= # [Brassard-Braunstein-Cleve 98] (T as a quantum computation),
= # [Braunstein-Kimble 98 a](T of continuous quantum variables),
= # [Collins 98] (Phys. Today),
= # [Pan-Bouwmeester-Weinfurter-Zeilinger 98],
= # [Garcia Alcaine 98 a] (review),
= # [Klyshko 98 c] (on the realization and meaning of T),
= # [Molotkov 98 a] (T of a single-photon wave packet),
= # [de Almeida-Maia-Villas Boas-Moussa 98] (T of atomic states with cavities),
= # [Ralph-Lam 98] (T with bright squeezed light),
= # [Horodecki-Horodecki-Horodecki 99 c] (general T channel, singlet fraction and quasi-distillation),
= # [Vaidman 98 c] (review of all proposals and experiments, and T in the many-worlds interpretation),
= # [Zubairy 98] (T of a field state),
= # [Nielsen-Knill-Laflamme 98] (complete quantum T using nuclear magnetic resonance),
= # [Stenholm-Bardroff 98] (T of N-dimensional states),
= # [Karlsson-Bourennane 98] (T using three-particle entanglement),
= # [Plenio-Vedral 98] (T, entanglement and thermodynamics),
= # [Ralph 98] (all optical quantum T),
= # [Maierle-Lidar-Harris 98] (T of superpositions of chirial amplitudes),
= # [Vaidman-Yoran 99] (methods for reliable T),
= # [Lutkenhaus-Calsamiglia-Suominen 99] (a never-failing measurement of the Bell operator in a two two-level bosonic system is impossible with beam splitters, phase shifters, delay lines, electronically switched linear elements, photo-detectors, and auxiliary bosons),
= # [Linden-Popescu 99] (bound entanglement and T),
= # [Molotkov-Nazin 99 b] (on T of continuous variables),
= # [Tan 99] (confirming entanglement in continuous variable quantum T),
= # [Villas Boas-de Almeida-Moussa 99] (T of a zero- and one-photon running-wave state by projection synthesis),
= # [van Enk 99] (discrete formulation of T of continuous variables),
= # [Milburn-Braunstein 99] (T with squeezed vacuum states),
= # [Ryff 99],
= # [Koniorczyk-Janszky-Kis 99] (photon number T),
= # [Bose-Knight-Plenio-Vedral 99] (proposal for T of an atomic state via cavity decay),
= # [Ralph-Lam-Polkinghorne 99] (characterizing T in optics),
= # [Maroney-Hiley 99] (T understood through the Bohm interpretation),
= # [Hardy 99 b] (a toy local theory in which cloning is not possible but T is),
= # [Parkins-Kimble 99] (T of the wave function of a massive particle),
= # [Marinatto-Weber 00 b] (which kind of two-particle states can be teleported through a three-particle quantum channel?),
= # [Bouwmeester-Pan-Weinfurter-Zeilinger 00] (high-fidelity T of independent qubits),
= # [Zeilinger 00 c],
= # [van Loock-Braunstein 00 a] (T of continuous-variable entanglement),
= # [Banaszek 00] (optimal T with an arbitrary pure state),
= # [Opatrny-Kurizki-Welsch 00] (improvement on T of continuous variables by photon subtraction via conditional measurement),
= # [Horoshko-Kilin 00] (T using quantum nondemolition technique),
= # [Murao-Plenio-Vedral 00] (T of quantum information to N particles),
= # [Li-Li-Guo 00] (probabilistic T and entanglement matching),
= # [Cerf-Gisin-Massar 00] (classical T of a qubit),
= # [DelRe-Crosignani-Di Porto 00] (scheme for total T),
= # [Kok-Braunstein 00 a] (postselected versus nonpostselected T using parametric down-conversion),
= # [Bose-Vedral 00] (mixedness and T),
= # [van Loock-Braunstein 00 b] (multipartite entanglement for continuous variables: A quantum T network),
= # [Braunstein-DAriano-Milburn-Sacchi 00] (universal T with a twist),
= # [Bouwmeester-Ekert-Zeilinger 00] (book on quantum information),
= # [Dur-Cirac 00 b] (multiparty T),
= # [Henderson-Hardy-Vedral 00] (two-state T),
= # [Motoyoshi 00] (T without Bell measurements),
= # [Vitali-Fortunato-Tombesi 00] (complete T with a Kerr nonlinearity),
= # [Galvao-Hardy 00 a] (building multiparticle states with T),
= # [Banaszek 00 a] (optimal T with an arbitrary pure state),
= # [Lee-Kim 00] (entanglement T via Werner states),
= # [Lee-Kim-Jeong 00] (transfer of nonclassical features in T via a mixed quantum channel),
= # [Zukowski 00 b] (Bell's theorem for the nonclassical part of the T process),
= # [Clausen-Opatrny-Welsch 00] (conditional T using optical squeezers),
= # [Grangier-Grosshans 00 a] (T criteria for continuous variables),
= # [Koniorczyk-Kis-Janszky 00],
= # [Gorbachev-Zhiliba-Trubilko-Yakovleva 00] (T of entangled states and dense coding using a multiparticle quantum channel),
= # [van Loock-Braunstein 00 d] (telecloning and multiuser quantum channels for continuous variables),
= # [Hao-Li-Guo 00](probabilistic dense coding and T),
= # [Zhou-Hou-Zhang 01] (T of S-level pure states by two-level EPR states),
= # [Trump-Brus-Lewenstein 01] (realistic T with linear optical elements),
= # [Werner 01 a] (T and dense coding schemes),
= # [Ide-Hofmann-Kobayashi-Furusawa 01] (continuous variable T of single photon states),
= # [Wang-Feng-Gong-Xu 01] (atomic-state T by using a quantum switch),
= # [Braunstein-Fuchs-Kimble-van Loock 01] (quantum versus classical domains for T with continuous variables),
= # [Bowen-Bose 01] (T as a depolarizing quantum channel),
= # [Shi-Tomita 02] (T using a W state),
= # [Agrawal-Pati 02] (probabilistic T),
= # [Yeo 03 a] (T using a three-qubit W state),
= # [Peres 03 b] (it includes a narrative of how Peres remembers that T was conceived).

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