about
Quantum robots and environmentsQuantum-Bayesian coherenceBiomimetic cloning of quantum observables.Quantum Communication Using Coherent Rejection Sampling.Creating a Superposition of Unknown Quantum States.Monitoring of the Process of System Information Broadcasting in Time.Objectivity in a noisy photonic environment through quantum state information broadcasting.Entanglement replication in driven dissipative many-body systems.No-broadcasting theorem and its classical counterpart.No-local-broadcasting theorem for multipartite quantum correlations.Generalized no-broadcasting theorem.Superbroadcasting of mixed states.Quantum key distribution in the Holevo limit.Quantum copying: Beyond the no-cloning theorem.Quantum cloningDistance measures to compare real and ideal quantum processesQuantifying CoherenceIntroducing the Qplex: a novel arena for quantum theoryQuantum teleportation using three-particle entanglementCriteria for continuous-variable quantum teleportationEntanglement versus noncommutativity in teleportationRealization of optimal disentanglement by teleportation via separable channelsFidelity of Gaussian Channels
P2860
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P2860
description
1996 nî lūn-bûn
@nan
1996年の論文
@ja
1996年学术文章
@wuu
1996年学术文章
@zh
1996年学术文章
@zh-cn
1996年学术文章
@zh-hans
1996年学术文章
@zh-my
1996年学术文章
@zh-sg
1996年學術文章
@yue
1996年學術文章
@zh-hant
name
Noncommuting mixed states cannot be broadcast.
@en
Noncommuting mixed states cannot be broadcast.
@nl
type
label
Noncommuting mixed states cannot be broadcast.
@en
Noncommuting mixed states cannot be broadcast.
@nl
prefLabel
Noncommuting mixed states cannot be broadcast.
@en
Noncommuting mixed states cannot be broadcast.
@nl
P2093
P2860
P1476
Noncommuting mixed states cannot be broadcast.
@en
P2093
P2860
P304
P356
10.1103/PHYSREVLETT.76.2818
P407
P577
1996-04-01T00:00:00Z
P698
P818
quant-ph/9511010