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Laser-Induced Fluorescence and Absorption Spectroscopy - Laser Physics | PHY 395M, Study notes of Physics

Material Type: Notes; Class: LASER PHYSICS; Subject: Physics; University: University of Texas - Austin; Term: Spring 2004;

Typology: Study notes

Pre 2010

Uploaded on 08/26/2009

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Download Laser-Induced Fluorescence and Absorption Spectroscopy - Laser Physics | PHY 395M and more Study notes Physics in PDF only on Docsity! Lagen bear, tre @, Vea A O La Sea S ectrosce Hafod Laser Spectroscopy 0) Laser — in duced Fhucrescence (LCF) pram Sunes Aet pho te dec to Sensitivity RB ‘ : 1e> mee F7 ae > ff A- 1? e > >» Lene Pil, CAinps/ 0 #) power outo fA ofodrod ae ee tes 3 bide ubtendkel sQ= 2 "by a ; é P Pal . “ ty z “Wande. caret OQ Absorption PrMersfy Sy Sigqrel al leader detector SES) KL Advantages f LIF low backgroud phe fecurrent ef tow ba ckeg rowel noise. ~My > suitable for detecting wea Je Sigoal ¢ From Very smal] hum bers atmo. Advantages for gqbhsorption spectrascepy _ Fer tases in which eptrcell depth ake, absorp tion 's more fensiAve than Fluorescance Che. Ca, measure hum barr f absor bin atoms fn kss cuewag hg tine) Essentially this is Aue to fact that fr ele each absorbed Phsta. results in only a Pordba bility ~ enn ‘ i having 9 detected plete, whereas va “absapiion Spectre Scopy each yhoten Is detectd as a “missing " ho tims Cron, The detected lager Leamr- Alse, abcerp tom Spe ctroscopy is shy hrly 2a 6 hem to set Sh Absorption in a ges — Doppler breadened Hii iba [Similay to what we discussed earlier in classical except Ge Satura ery effects ) won, -«h =Pe -. == — Ia p Rue —l— |b> © LK orden +o talee enaatawtae i haf oenee tie f {osena, sh FS neces to find methods fo remove Dopp ba effect. Mest commen methods | (©) Atomic bean spechoscory ler Free Spe. aa bere diver, 1 — 1 . ae ae TE et ladon L ecu A narths ete (Cx n be ) Deppler shite ev oO => Depp lepoGee. residual Deppler width - & eg ke x | Ge ar 107 an Px wi dite © Twexphoten spectrscopy _ : Doppler shift ve } -é2s Pons) Hor is aie hwo °F osu: maps ya re ° a ley die. ia enp Ty se PK vo, By 2 ° Two ~photon reson \, ia D= 2w,—- (wr -kyv) —(wrky) Ly, F; Zi 0 Is Oy = = 2W,y~ ZW a jy be shitth. @ Saturation Cine) Spee Pee I<Ts plimp _leten LL. 2 Te probe absorption coefficie +e Since probe Tels) probe has Title ellect om populations q(x) and 7,Cx), Pump becn dees affect populations. Hence oo % =f fro -7,0)) CN dx ee el An -® populations crosS- Section boy probe bea . established by has opposite Deppler pump beam chif+ te pumy bean , Com Show? _ (, 2) Xe = i GS (A) Pi ae S Bor (we/2 A Ww = a it A EE = owt — broadtued : ( Fs ) P Jin-ew folHe, f= i eee Siem (1441+ Fa) Sub- Doppler resglubion ) with on" In { et fect x) opal ati cpulation it i) ies 1 phe. Cele fob . A W, ¥ 2 = lo MHe, net 16He-l faba of wie, Sant populations - 3 decreased probe absovy tim Oo exact vesenentee, b=-O0. (due te Shura Coiaced ge eS
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