Spectroscopy of Rb - crossover peaks more intense?

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SUMMARY

The discussion focuses on the atomic spectroscopy of Rubidium (Rb) using saturated absorption spectroscopy, specifically addressing the intensity of crossover peaks compared to other spectral peaks. Crossover peaks occur when the pump laser excites atoms from one transition's Gaussian tail that overlaps in frequency with atoms interacting with the probe beam from a different transition's Gaussian tail. C. J. Foot's "Atomic Physics" provides a detailed explanation of this phenomenon. Experimentation with pump beam power may help control the relative intensities of pure transitions and crossover peaks, with power broadening being a contributing factor.

PREREQUISITES
  • Saturated absorption spectroscopy
  • Atomic spectroscopy principles
  • Understanding of Gaussian distribution in spectral lines
  • Knowledge of power broadening effects
NEXT STEPS
  • Read C. J. Foot's "Atomic Physics" for detailed explanations of crossover resonance
  • Experiment with varying pump beam power in saturated absorption setups
  • Investigate the effects of power broadening on spectral peak intensities
  • Explore advanced techniques in atomic spectroscopy for enhanced peak resolution
USEFUL FOR

Researchers and students in atomic physics, optical spectroscopy practitioners, and anyone interested in the nuances of saturated absorption spectroscopy and its applications in studying atomic transitions.

Mattcr_95
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Hi,

I am currently looking into the atomic spectroscopy of Rb using saturated absorption spectroscopy. So far I can observe the crossover peaks with hyperfine splitting. I am aware of why crossover peaks occur however do not understand why these transitions are so much more intense than the other peaks?

Thanks
 
I know how saturation spectroscopy works but I am not sure which peaks you are referring by crossover peaks.
 
gre_abandon said:
I know how saturation spectroscopy works but I am not sure which peaks you are referring by crossover peaks.

He means the peaks caused when the pump laser excites atoms from one transition's Gaussian tail that overlap in frequency with atoms interacting with the probe beam from the Gaussian tail of a different transition. C. J. Foot explains it and uses the term crossover resonance in Chapter 7 or so of Atomic Physics.

Unfortunately I don't remember why the crossover peaks appear bigger. If you have access to such a setup, you may want to experiment with the power of the pump beam to see if you can't control the relative sizes of the pure transitions and the crossovers. Power broadening may be part of the answer.
 

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