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Time frequency distributions of Optical sources (II): externally modulated semiconductor lasers
Abstract
We extend a time frequency framework previously developed for directly modulated lasers to external modulation of the continuous wave output of a 1550 nm DFB laser described by Langevin rate equations. Four modulators are considered an InP electro absorption modulator, a LiNbO3 dual drive Mach Zehnder modulator, a dual parallel Mach Zehnder modulator and a silicon carrier depletion modulator
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BibTeX
@misc{capmany2026time,
title = {{Time frequency distributions of Optical sources (II): externally modulated semiconductor lasers}},
author = {José Capmany},
howpublished = {arXiv},
year = {2026},
month = oct,
doi = {10.48550/arxiv.2610.06149},
eprint = {2610.06149},
archivePrefix = {arXiv},
url = {https://arxiv.org/abs/2610.06149},
}
RIS
TY - UNPB
TI - Time frequency distributions of Optical sources (II): externally modulated semiconductor lasers
AU - José Capmany
PY - 2026
DA - 2026/10/05
PB - arXiv
DO - 10.48550/arxiv.2610.06149
UR - https://arxiv.org/abs/2610.06149
AB - We extend a time frequency framework previously developed for directly modulated lasers to external modulation of the continuous wave output of a 1550 nm DFB laser described by Langevin rate equations. Four modulators are considered an InP electro absorption modulator, a LiNbO3 dual drive Mach Zehnder modulator, a dual parallel Mach Zehnder modulator and a silicon carrier depletion modulator
ER -