2016
DOI: 10.1038/srep36914
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Detection-dependent six-photon Holland-Burnett state interference

Abstract: The NOON state, and its experimental approximation the Holland-Burnett state, have important applications in phase sensing measurement with enhanced sensitivity. However, most of the previous Holland-Burnett state interference (HBSI) experiments only investigated the area of the interference pattern in the region immediately around zero optical path length difference, while the full HBSI pattern over a wide range of optical path length differences has not yet been well explored. In this work, we experimentally… Show more

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Cited by 24 publications
(18 citation statements)
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“…Our results, on the one hand, provide a new characteristic of multi-photon interference [22,24,25,[27][28][29][30][31], and, on the other hand, they may inspire investigation of a more foundational character, cf. the different view on wave-particle duality in first and second quantization [8,9,32,33].…”
mentioning
confidence: 76%
“…Our results, on the one hand, provide a new characteristic of multi-photon interference [22,24,25,[27][28][29][30][31], and, on the other hand, they may inspire investigation of a more foundational character, cf. the different view on wave-particle duality in first and second quantization [8,9,32,33].…”
mentioning
confidence: 76%
“…Superconducting nanowire single photon detectors (SSPDs) 10 are promising for HOM observation because of the high DE of ~90% 11 , low DCR of a few counts/s 12 , and short timing jitter as low as ~20 ps with a Gaussian instrumental response 13 . Successful observations of HOM interference using SSPDs have been demonstrated 3,4,9,14,15 . Meanwhile, the measured timing jitter of SSPD systems still has potential for improvement by suppressing external contributions other than the intrinsic jitter of detector itself, such as the contributions of the low noise amplifier and time correlated single-photon counting (TCSPC) module.…”
Section: Textmentioning
confidence: 99%
“…最后一步, (2N-1)步的操作: [27] 已证明在量子电动力学(CQED)中, U x y ( ; ) qudit Bell和qubit-qutrit Bell态 [28][29][30][31][32][33][34][35] ; UCNOT(c;t)表示通常 的qubit-qubit CNOT门, UCNOT(c;t (N) )表示方程(8)所示的 qubit-qudit CNOT门 [13,[36][37][38] ; UC-V(c (N) ;t)表示方程(7)所示 qudit-qubit受控幺正门 [13,[36][37][38] ; U x y ( , ) i j 表示方程(27)所 示2-qutrit的条件交换门 [27,28] . 显然, 相比Eisert等人 [15] 最初提出的方案和本课题 组 [16] 2011年提出的方案, 本文方案所需的两体操作数 量较少, 且不需要辅助系统.…”
Section: 第4步 T操作unclassified