2022
DOI: 10.1103/physrevapplied.17.054021
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Multinode State Transfer and Nonlocal State Preparation via a Unidirectional Quantum Network

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Cited by 4 publications
(5 citation statements)
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“…Quantum entanglement serves as a fundamental element for quantum computation and quantum communication [59][60][61]. The generation and distribution of entangled states have long been the main topic in the field of quantum information processing [12,14,[38][39][40][41]. In linear optical systems, entanglement can be prepared by certain bosonic transformation such as beam splitter.…”
Section: Entanglement Preparationmentioning
confidence: 99%
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“…Quantum entanglement serves as a fundamental element for quantum computation and quantum communication [59][60][61]. The generation and distribution of entangled states have long been the main topic in the field of quantum information processing [12,14,[38][39][40][41]. In linear optical systems, entanglement can be prepared by certain bosonic transformation such as beam splitter.…”
Section: Entanglement Preparationmentioning
confidence: 99%
“…For example, it plays a crucial role in the problem of Bose samplings [1][2][3][4][5], which is of particular interest in the study of near-term platform for photonic quantum computing [6]. The linear bosonic transformation can be effectively realized by optical beam splitters and wave plates in optical systems under the protocol raised by Knill, Laflamme and Milburn [7][8][9], or by controllable pulse manipulation in superconductor-waveguide systems [10][11][12][13][14][15]. Experimental progresses in this direction have facilitated the development of various quantum information tasks, including quantum state transfer (QST), entanglement preparation (EP) and entanglement distribution [12][13][14][15][16][17].…”
Section: Introductionmentioning
confidence: 99%
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“…( 9) reduces to the dark-state condition employed for identifying control pulses for single-mode quantum state transfer schemes [33,[50][51][52][53][54][55] (see also Ref. [56] for a preliminary extension to multimode setups). In the Supplemental Material [46], we show that satisfying this generalized set of dark-state conditions for all l ¼ 1; …; N is not only necessary, but also sufficient to obtain G BA ðt f ; t 0 Þ ≃ U and G BB ðt f ; t 0 Þ ≃ 0 for sufficiently long t f .…”
mentioning
confidence: 99%