The measurement of 3s energy levels of atomic lithium

碩士 === 國立清華大學 === 物理學系 === 95 === To determined the $3$s energy levels of lithium isotopes, a $735$ nm Ti:Sapphire laser is used to excite the ground state atomic lithium from a atomic beam system. The laser frequency is measured simultaneously by optical frquency comb, which gives the accuracy to $...

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Main Authors: Jwo-Sy Chen, 陳倬思
Other Authors: Yi-Wei Liu
Format: Others
Language:en_US
Published: 2007
Online Access:http://ndltd.ncl.edu.tw/handle/35567323886192413729
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spelling ndltd-TW-095NTHU51980472015-10-13T16:51:16Z http://ndltd.ncl.edu.tw/handle/35567323886192413729 The measurement of 3s energy levels of atomic lithium Themeasurementof3senergylevelsofatomiclithium Jwo-Sy Chen 陳倬思 碩士 國立清華大學 物理學系 95 To determined the $3$s energy levels of lithium isotopes, a $735$ nm Ti:Sapphire laser is used to excite the ground state atomic lithium from a atomic beam system. The laser frequency is measured simultaneously by optical frquency comb, which gives the accuracy to $10^{-12}$ level. The excitation laser is stabilized by phase-locking to a specific comb line. The induced fluorescences spectra of $2$p-$2$s decay channel are fitted to a Voigt function with a Gaussian background to decide the transition line centers. The best signal-to-noise ratio of the transition spectrum is about $200$. The measured transition centers are $815\,618\,181.26(48)$ MHz and $815\,606 \,729.8(24)$ MHz for $^7$Li and $^6$Li $2$s-$3$s transitions respectively, which is improved by an order of magnitude for \,$^7$Li. However, The hyperfine structure constants, $93.73(48)$ MHz for \,$^7$Li and $36.0(35)$ MHz for \,$^6$Li, show the discrepancy with previous measurements \cite{Bushaw2003,Ewald2004}. Yi-Wei Liu 劉怡維 2007 學位論文 ; thesis 34 en_US
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description 碩士 === 國立清華大學 === 物理學系 === 95 === To determined the $3$s energy levels of lithium isotopes, a $735$ nm Ti:Sapphire laser is used to excite the ground state atomic lithium from a atomic beam system. The laser frequency is measured simultaneously by optical frquency comb, which gives the accuracy to $10^{-12}$ level. The excitation laser is stabilized by phase-locking to a specific comb line. The induced fluorescences spectra of $2$p-$2$s decay channel are fitted to a Voigt function with a Gaussian background to decide the transition line centers. The best signal-to-noise ratio of the transition spectrum is about $200$. The measured transition centers are $815\,618\,181.26(48)$ MHz and $815\,606 \,729.8(24)$ MHz for $^7$Li and $^6$Li $2$s-$3$s transitions respectively, which is improved by an order of magnitude for \,$^7$Li. However, The hyperfine structure constants, $93.73(48)$ MHz for \,$^7$Li and $36.0(35)$ MHz for \,$^6$Li, show the discrepancy with previous measurements \cite{Bushaw2003,Ewald2004}.
author2 Yi-Wei Liu
author_facet Yi-Wei Liu
Jwo-Sy Chen
陳倬思
author Jwo-Sy Chen
陳倬思
spellingShingle Jwo-Sy Chen
陳倬思
The measurement of 3s energy levels of atomic lithium
author_sort Jwo-Sy Chen
title The measurement of 3s energy levels of atomic lithium
title_short The measurement of 3s energy levels of atomic lithium
title_full The measurement of 3s energy levels of atomic lithium
title_fullStr The measurement of 3s energy levels of atomic lithium
title_full_unstemmed The measurement of 3s energy levels of atomic lithium
title_sort measurement of 3s energy levels of atomic lithium
publishDate 2007
url http://ndltd.ncl.edu.tw/handle/35567323886192413729
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