1990
DOI: 10.1109/50.59179
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DBR active optical filters: transfer function and noise characteristics

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Cited by 29 publications
(5 citation statements)
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“…We assume that K 12 cm-' is feasible. The conclusion that short active and phase sections and weak gratings should be employed, is consistent with the results of Kazovsky et al [12].…”
Section: Improved Devicessupporting
confidence: 89%
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“…We assume that K 12 cm-' is feasible. The conclusion that short active and phase sections and weak gratings should be employed, is consistent with the results of Kazovsky et al [12].…”
Section: Improved Devicessupporting
confidence: 89%
“…The last factor in (13) accounts for scattering losses, etc. The first term in (12) corresponds to the amplified signal, the second term to resonantly amplified spontaneous emission, and the terms on the third line correspond to ASE from all other modes within the gain curve. They are approximated as free, traveling wave modes.…”
Section: Noise Properties Measured and Calculated Bermentioning
confidence: 99%
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“…Tunable DBR Filter/Photodetector Injecting current into the active layer of DBR filter, the central wavelength can be tuned due to the decrease ofthe refractive index [20][21][22][23][24]. To achieve polarization independent tunable DBR filter, a symmetric waveguide core was fabricated using buried heterostructure [25] to get the same effective refractive indices for both the TE and TM modes.…”
Section: 2mentioning
confidence: 99%
“…Kazovsky et al [6] have shown that two drawbacks of a conventional DBR device, a multilobe transfer function, and a small gain can be alleviated by reduction of the grating coupling coefficient and the physical length of one or the two sections. This technique can lead to devices having a gain of 35 dB, sidelobe suppression of 32 dB and bandwidth as narrow as 1 GHz.…”
Section: Introduction Wavelength Filter Is a Key Component For Wave-mentioning
confidence: 98%