Level%20crossing%20spectroscopy - PowerPoint PPT Presentation

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Level%20crossing%20spectroscopy

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LASERs used for optical pumping which allows molecular spectroscopy. Topics of Discussion ... sub-levels.Superpsition of two different routes (J',M) - (Jf,M) ... – PowerPoint PPT presentation

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Title: Level%20crossing%20spectroscopy


1
Level crossing spectroscopy
  • rudresh ghosh
  • saurish chakrabarty

2
Introduction
  • Well known Doppler-free technique
  • Pre laser era atomic spectroscopy
  • LASERs used for optical pumping which allows
    molecular spectroscopy

3
Topics of Discussion
  • Basic principle and exptl setup
  • Hanle effect
  • Quantum mechanical description
  • Advantages disadvantages
  • Modifications

4
Basic principle and exptl setup
Schematic expterimental setup for level crossing
spectroscopy
5
Basic principle and exptl setup
  • Sample placed in uniform magnetic field
  • Illuminated by polarized light
  • Emits fluorescence
  • Shape of signal Ifl(B) gives gt

6
Important equations
  • E(t)E(0)exp-(iw12g/2)(t-to)
  • wLgjmoB/h
  • I(B,a,t)IOexp-g(t-to)cos2wL(t-tO)-a
  • I(B,a)R-8?t IOexp-g(t-to)cos2wL(t-tO)-adtO
  • IOR1/g(gcos2a2wLsin2a)/(g24wL2)
    /2
  • I(B)(I0R/2g)1-(1/(1(2gm0B/hg)2)
  • DB1/2hg/gmo
  • h/mogt

7
Hanle Effect
  • In case of Zeeman subl-evels of a degenewrate J
    level, the M levels cross each other at B0,when
    the field is tuned from ve to ve values. This
    is called Hanle effect or zero-field level
    crossing.

8
Quantum mechanical description
  • Level scheme for optical pumping of Zeeman
    levels by light polarised in y-direction.Each of
    the two excited Zeeman levels can decay into
    three final state sub-levels.Superpsition of two
    different routes (J,M) -gt(Jf,M) generates
    interference effects

9
Quantum mechanical description
  • I2gtx-1/21/2aM1IM1gtaM-1IM-1gt
  • I2gty-i/21/2aM1IM1gt-aM-1IM-1gt
  • y2(t)e-g(t-t0)/2 e-iH(t-t0)/h y2(t0)
  • e-g(t-t0)/2 e-i(E0mBgMB)(t-t0)/hIy2gtxsinmBgB(
    t-t0)/h Iy2gtycosmBgB(t-t0)/h
  • I(Ex,t)cexp(-gt)sin2(mBgBt/h)
  • Iy(Ex)(ct/2)(2mBgBt/h)2/1(2mBgBt/h)2

10
Advantages
  • Compared to other Doppler free techniques needs
    simple exptl arrangement
  • Sign of dispersion shaped Hanle curve determines
    the sign of the Lande g factor.

11
Disadvantages
  • There is change in absorption profile with change
    in magnetic field.Laser bandwidth must be
    sufficiently large so that all Zeeman components
    can absorb the laser radiation independent of the
    field strength B.Should not be so large so that
    simultaneous excitations of different closely
    spaced transitions occur.
  • Large magnetic fields are required for Hanle
    signals from short lived molecular levels with
    small g.

12
Modifications
  • To improve signal to noise ratio a method known
    as stimulated level crossing spectroscopy is used
  • Use of electric fields instead of magnetic fields
  • Studying molecules with simultaneous electric and
    magnetic level crossing spectroscopy give the
    value of g and t simultaneously.

13
Thank you
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