1998
DOI: 10.1109/3.661447
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Analysis of polarization-dependent gain in fiber amplifiers

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Cited by 14 publications
(5 citation statements)
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“…For optoelectronic devices working in the mid-infrared 2-5 µm wavelengths, the InAs-based heterostructure has been adopted because of its narrow bandgap (0.36 eV at room temperature). Wang et al [13] have demonstrated a high-quality 2.2 µm InAs/InGaAs/InP highly strained multiple quantum well (QW) laser grown by gas source molecular beam epitaxy. Recently, it has been shown that a better heterointerface can be achieved by replacing InAs with InAsN alloys since nitrogen atoms are smaller than arsenic [14].…”
Section: Introductionmentioning
confidence: 99%
“…For optoelectronic devices working in the mid-infrared 2-5 µm wavelengths, the InAs-based heterostructure has been adopted because of its narrow bandgap (0.36 eV at room temperature). Wang et al [13] have demonstrated a high-quality 2.2 µm InAs/InGaAs/InP highly strained multiple quantum well (QW) laser grown by gas source molecular beam epitaxy. Recently, it has been shown that a better heterointerface can be achieved by replacing InAs with InAsN alloys since nitrogen atoms are smaller than arsenic [14].…”
Section: Introductionmentioning
confidence: 99%
“…However, if one polarization saturates the amplifier, a slight excess gain is left over in the other polarization. Noise can grow in this polarization and affect the system performance [Wang et al, 1998].…”
Section: Edf Co-operative Up-conversionmentioning
confidence: 99%
“…Section 3 describes the growth of InAs/InGaAs MQWs and the fabrication of the device. Although the use of highly strained (3.2%) InAs limits the layer thickness, 15,16) we have successfully achieved the stable growth of a highly strained InAs well with a layer as thick as 5 nm. A thicker well layer in a low electric field results in a deeper quantum level in the well, producing a cutoff wavelength as large as 2.4 mm.…”
Section: Introductionmentioning
confidence: 97%