2017
DOI: 10.7566/jpsj.86.054401
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Impact of Backscattering in Silicon Micro-ring Resonators on Photon Pair Generation

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Cited by 4 publications
(3 citation statements)
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“…The fitted slopes of six combinations were 2.03, 1.91, 1.91, 1.94, 1.94 and 1.92. All the slopes are close to 2, showing that under all the channel combinations the main contribution of the coincident counts is due to the photon pairs generated by SFWM [11] . At the pump level of 0.59mW, the CCRs of ch12 and ch34 reached ~550Hz, while the average CCR of other four combinations was ~72Hz.…”
Section: (B)mentioning
confidence: 68%
See 1 more Smart Citation
“…The fitted slopes of six combinations were 2.03, 1.91, 1.91, 1.94, 1.94 and 1.92. All the slopes are close to 2, showing that under all the channel combinations the main contribution of the coincident counts is due to the photon pairs generated by SFWM [11] . At the pump level of 0.59mW, the CCRs of ch12 and ch34 reached ~550Hz, while the average CCR of other four combinations was ~72Hz.…”
Section: (B)mentioning
confidence: 68%
“…It can be seen that for all the six combinations, there are obvious coincident counts recorded, which rise with increasing pump level. Ch12 and ch34 respected the CCR of CCW and CW respectively, while the other four came from photons induced by backscattering, which is mainly caused by the roughness of waveguide sidewall [11] . The fitted slopes of six combinations were 2.03, 1.91, 1.91, 1.94, 1.94 and 1.92.…”
Section: (B)mentioning
confidence: 99%
“…Typically, their transmission displays Lorentzianshaped resonant peaks, reaching a minimum when the ring circumference is an integer multiple of the wavelength [12]. However, these devices are vulnerable to backscatter [13].…”
Section: Introductionmentioning
confidence: 99%