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Volumn 80, Issue 20, 2009, Pages

Electronic entanglement via quantum Hall interferometry in analogy to an optical method

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EID: 77954738636     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.80.201312     Document Type: Article
Times cited : (10)

References (32)
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    • We identify the two levels of each qubit with the pair of outgoing channels at each side of the interferometer (along which only one particle electron or hole propagates). Defining the upper state of each qubit as the electron excitation, |1« = C (L,R ) 1 † | 0̄ », and the lower state as the hole one, |0« = C (L,R ) 2 | 0̄ », the first two terms in Eq. read as t1 t2*- | 10 « - r1 r2*| 01 ».
    • We identify the two levels of each qubit with the pair of outgoing channels at each side of the interferometer (along which only one particle electron or hole propagates). Defining the upper state of each qubit as the electron excitation, |1« = C (L,R ) 1 † | 0̄ », and the lower state as the hole one, |0« = C (L,R ) 2 | 0̄ », the first two terms in Eq. read as t1 t2*- | 10 « - r1 r2*| 01 ».
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    • note
    • The U L and U R mixing matrices can absorb the kinetic/magnetic phases acquired by the electrons (and holes) along their way from BS-1 and BS-2 to drains, so we do not need to consider them explicitly. Notice that the mixing can be performed either by controlling the transmission amplitude of BS-L and BS-R by modifying the Aharonov-Bohm flux through the interferometer or by introducing local electric gates that modify the length of selected paths toward the left and/or right side of the interferometer.
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* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.