Study on Difference Frequency Generation Light Source

碩士 === 國立清華大學 === 光電工程研究所 === 99 === In this thesis, we observe the saturation spectrum of N2O 0001←0000 fundamental band R(10) transition by a CW mid-infrared MgO:PPLN-based difference frequency generation (DFG) source pumped by a Ti:Sapphire laser and a Nd:YAG laser. The absolute frequency of...

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Main Authors: Lan, Tzu-Kai, 藍子凱
Other Authors: Shy, Jow-Tsong
Format: Others
Language:zh-TW
Published: 2011
Online Access:http://ndltd.ncl.edu.tw/handle/20060376436555046305
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spelling ndltd-TW-099NTHU51241462015-10-13T20:23:00Z http://ndltd.ncl.edu.tw/handle/20060376436555046305 Study on Difference Frequency Generation Light Source 差頻光源之研究 Lan, Tzu-Kai 藍子凱 碩士 國立清華大學 光電工程研究所 99 In this thesis, we observe the saturation spectrum of N2O 0001←0000 fundamental band R(10) transition by a CW mid-infrared MgO:PPLN-based difference frequency generation (DFG) source pumped by a Ti:Sapphire laser and a Nd:YAG laser. The absolute frequency of R(10) transition is also determined by the femtosecond optical frequency comb (OFC). We present two methods to stabilize the frequency of DFG source. Method 1: Ti:S scan in which we stabilize the frequency of Nd:YAG laser on the a10 component, R(56) 32-0 transition iodine molecule 127I2, and the frequency of DFG source is scanned and locked by tuning the frequency of Ti:Sapphire laser. Method 2: YAG scan in which we stabilize the frequency of Ti: Sapphire laser using a thermally isolated Fabry-Perot cavity, and the frequency of the DFG source is scanned and locked by tuning the frequency of the Nd:YAG laser. The absolute frequency of N2O transition is equal to the difference of two laser frequencies. In Ti:S scan method, we assume that the frequency of Nd:YAG laser is a known value, so we only measure the frequency of Ti:Sapphire laser by the OFC. And in YAG scan method, we have to measure the frequencies of Ti:Sapphire laser and Nd:YAG laser simultaneously. However, in Ti:S scan, the frequency of Nd:YAG laser isn’t a fixed value actually and it is different for different frequency locking condition. After measuring the Nd:YAG laser, the frequency difference of the absolute frequency measurements using Ti:S scan and YAG scan is approximate 1 kHz. Due to the monolithic non-planar ring oscillator structure of Nd:YAG laser, its frequency stability is better than Ti:Sapphire laser. Our system has better resolution by adopting the YAG scan method. In addition, we have to improve the feedback system to increase the accuracy in measuring the absolute frequency. Shy, Jow-Tsong 施宙聰 2011 學位論文 ; thesis 62 zh-TW
collection NDLTD
language zh-TW
format Others
sources NDLTD
description 碩士 === 國立清華大學 === 光電工程研究所 === 99 === In this thesis, we observe the saturation spectrum of N2O 0001←0000 fundamental band R(10) transition by a CW mid-infrared MgO:PPLN-based difference frequency generation (DFG) source pumped by a Ti:Sapphire laser and a Nd:YAG laser. The absolute frequency of R(10) transition is also determined by the femtosecond optical frequency comb (OFC). We present two methods to stabilize the frequency of DFG source. Method 1: Ti:S scan in which we stabilize the frequency of Nd:YAG laser on the a10 component, R(56) 32-0 transition iodine molecule 127I2, and the frequency of DFG source is scanned and locked by tuning the frequency of Ti:Sapphire laser. Method 2: YAG scan in which we stabilize the frequency of Ti: Sapphire laser using a thermally isolated Fabry-Perot cavity, and the frequency of the DFG source is scanned and locked by tuning the frequency of the Nd:YAG laser. The absolute frequency of N2O transition is equal to the difference of two laser frequencies. In Ti:S scan method, we assume that the frequency of Nd:YAG laser is a known value, so we only measure the frequency of Ti:Sapphire laser by the OFC. And in YAG scan method, we have to measure the frequencies of Ti:Sapphire laser and Nd:YAG laser simultaneously. However, in Ti:S scan, the frequency of Nd:YAG laser isn’t a fixed value actually and it is different for different frequency locking condition. After measuring the Nd:YAG laser, the frequency difference of the absolute frequency measurements using Ti:S scan and YAG scan is approximate 1 kHz. Due to the monolithic non-planar ring oscillator structure of Nd:YAG laser, its frequency stability is better than Ti:Sapphire laser. Our system has better resolution by adopting the YAG scan method. In addition, we have to improve the feedback system to increase the accuracy in measuring the absolute frequency.
author2 Shy, Jow-Tsong
author_facet Shy, Jow-Tsong
Lan, Tzu-Kai
藍子凱
author Lan, Tzu-Kai
藍子凱
spellingShingle Lan, Tzu-Kai
藍子凱
Study on Difference Frequency Generation Light Source
author_sort Lan, Tzu-Kai
title Study on Difference Frequency Generation Light Source
title_short Study on Difference Frequency Generation Light Source
title_full Study on Difference Frequency Generation Light Source
title_fullStr Study on Difference Frequency Generation Light Source
title_full_unstemmed Study on Difference Frequency Generation Light Source
title_sort study on difference frequency generation light source
publishDate 2011
url http://ndltd.ncl.edu.tw/handle/20060376436555046305
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