Characterization of a Passive Mode Locked Ti-sapphire Laser With a Strained Quantum Well Saturable Bragg Reflector
碩士 === 國立交通大學 === 光電工程所 === 88 === Abstract We demonstrate mode-locking of femtosecond Ti-sapphire laser with a strained quantum well saturable Bragg reflector (SSBR). Two strained quantum wells were used as the absorbing layer. Self starting 110fs pulse tunable from 780 to 815nm were gen...
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ndltd-TW-088NCTU06140472016-07-08T04:22:41Z http://ndltd.ncl.edu.tw/handle/94883796944327979925 Characterization of a Passive Mode Locked Ti-sapphire Laser With a Strained Quantum Well Saturable Bragg Reflector 利用扭曲量子井布拉格式飽和吸收鏡之被動鎖模鈦藍寶石雷射特性之研究 Jer-tsong Chen 陳哲聰 碩士 國立交通大學 光電工程所 88 Abstract We demonstrate mode-locking of femtosecond Ti-sapphire laser with a strained quantum well saturable Bragg reflector (SSBR). Two strained quantum wells were used as the absorbing layer. Self starting 110fs pulse tunable from 780 to 815nm were generated in a X-folded cavity with an average output power of 800mW at a pulse repetition rate of 93MHz.We have achieved a mode locking build up time only 20us, using the SSBR to initiate the pulse formation. By time gated system, we found that the mode locked spectrum grow up faster than CW spectrum when the buildup time is shorter than 40us. When the buildup time is larger than 40us, the CW spectrum grow up faster than mode locked spectrum. Ci-Ling Pan 潘犀靈 2000 學位論文 ; thesis 45 zh-TW |
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碩士 === 國立交通大學 === 光電工程所 === 88 === Abstract
We demonstrate mode-locking of femtosecond Ti-sapphire laser with a strained quantum well saturable Bragg reflector (SSBR). Two strained quantum wells were used as the absorbing layer. Self starting 110fs pulse tunable from 780 to 815nm were generated in a X-folded cavity with an average output power of 800mW at a pulse repetition rate of 93MHz.We have achieved a mode locking build up time only 20us, using the SSBR to initiate the pulse formation.
By time gated system, we found that the mode locked spectrum grow up faster than CW spectrum when the buildup time is shorter than 40us. When the buildup time is larger than 40us, the CW spectrum grow up faster than mode locked spectrum.
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Ci-Ling Pan |
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Ci-Ling Pan Jer-tsong Chen 陳哲聰 |
author |
Jer-tsong Chen 陳哲聰 |
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Jer-tsong Chen 陳哲聰 Characterization of a Passive Mode Locked Ti-sapphire Laser With a Strained Quantum Well Saturable Bragg Reflector |
author_sort |
Jer-tsong Chen |
title |
Characterization of a Passive Mode Locked Ti-sapphire Laser With a Strained Quantum Well Saturable Bragg Reflector |
title_short |
Characterization of a Passive Mode Locked Ti-sapphire Laser With a Strained Quantum Well Saturable Bragg Reflector |
title_full |
Characterization of a Passive Mode Locked Ti-sapphire Laser With a Strained Quantum Well Saturable Bragg Reflector |
title_fullStr |
Characterization of a Passive Mode Locked Ti-sapphire Laser With a Strained Quantum Well Saturable Bragg Reflector |
title_full_unstemmed |
Characterization of a Passive Mode Locked Ti-sapphire Laser With a Strained Quantum Well Saturable Bragg Reflector |
title_sort |
characterization of a passive mode locked ti-sapphire laser with a strained quantum well saturable bragg reflector |
publishDate |
2000 |
url |
http://ndltd.ncl.edu.tw/handle/94883796944327979925 |
work_keys_str_mv |
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