2018
DOI: 10.1364/ol.43.003806
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Bounding the outcome of a two-photon interference measurement using weak coherent states

Abstract: The interference of two photons at a beam splitter is at the core of many quantum photonic technologies, such as quantum key distribution or linear-optics quantum computing. Observing high-visibility interference is challenging because of the difficulty of realizing indistinguishable single-photon sources. Here, we perform a two-photon interference experiment using phase-randomized weak coherent states with different mean photon numbers. We place a tight upper bound on the expected coincidences for the case wh… Show more

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Cited by 17 publications
(15 citation statements)
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References 16 publications
(27 reference statements)
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“…In the classical-light HOM-type experiment, the maximum visibility bound limited to 50% is only partly considered to be due to the photonnumber distribution of the light source itself. In fact, the limited visibility is the only cause of the  coincidence-detection contribution arising from the path-entangled state, which is intrinsic for the two input photons only when not considering multi-photon inputs 46,49 . At the two MZI-output ports shown in Fig.…”
Section: Resultsmentioning
confidence: 99%
“…In the classical-light HOM-type experiment, the maximum visibility bound limited to 50% is only partly considered to be due to the photonnumber distribution of the light source itself. In fact, the limited visibility is the only cause of the  coincidence-detection contribution arising from the path-entangled state, which is intrinsic for the two input photons only when not considering multi-photon inputs 46,49 . At the two MZI-output ports shown in Fig.…”
Section: Resultsmentioning
confidence: 99%
“…In Recent years, focal shaping of tight-focusing of laser beams such as highly confined focal spot/hole with extended focal depth, multiple focal spots, optical bubble etc., has important applications in high-density optical data storage [1], laser micro/nano-processing [2], particle and electron acceleration [3], super-resolution scanning confocal microscopy [4] and optical trapping [5]. The intensity distribution of the focal structure in the focal region has been frequently discussed [6][7][8][9][10][11][12][13]. To produce different types of intensity distribution in the focal plane one may insert a physical mask in the pupil plane of the objective [14][15][16][17][18].…”
Section: Introductionmentioning
confidence: 99%
“…In this paper, based on the recently proposed technique to characterize linear optical networks using non-ideal input states [21][22][23][24], we propose a method to characterize a linear optical BSA using WCP. In particular, we present a method to deduce the BSA result for ideal single-photon input states using the experimental data with WCP.…”
Section: Introductionmentioning
confidence: 99%