Photo-associative Ionization in Rb
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Photo-associative Ionization in Rb
Stimulated Adiabatic Rapid Passage:STIRAP, the untold story
Marc TrachyMudessar Shah, Alina Gearba,
Hyounguk Jang, Larry Weaver, Brett DePaola
5S1/2 F=2
5P3/2 F=3
4D5/2 F=?
780 nm
1529 nm
Relevant Levels of 87Rb
L2
L1
Description of STIRAP
Want to see time evolution!
If No Decay
Time Evolution Theory
But can we SEE it?
Motivation
•Toy system for (for example) KLS
•Coherent control is hot
•Group satisfaction
•Technical Improvements•EDFA (Thanks LUMOS!)•Delay control•Detector replacement
Experimental Setup
4d
5p
5s
5S1/2 F=2
5P3/2 F=3
4D5/2 F=?
780 nm
1529 nm
4D5/2
5S1/2
5P3/2
L1
L2
30 ns
L2
L1
4D5/2
5S1/2
5P3/2
L1
L2
4D5/2
5S1/2
5P3/2
L1
L2
Theory (Gaussian Pulses)
Theory
• Density matrix formalism• Gaussian pulses• Zero linewidth lasers• Individual atoms
– No collisions– No rescattering of radiation
• Approximations– Rotating wave– Dipole– Near resonance (keeping it to 3 levels)
Speculation on agreement
• Radiation trapping
• Polarization (mF)
• Hyperfine separation vs detuning
• Intuitive case more like CW or incoherent
• Even a Toy system holds questions– Toys can be complicated
• Need more levels in theory• Ready for more realistic toy systems
– with CW lasers– KLS
Lessons