Paschen notation in atomic spectroscopy

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SUMMARY

This discussion focuses on the use of Paschen notation in atomic spectroscopy, particularly for electronic excitation in Xenon. Paschen notation is essential for representing excited states of inert gases, with specific examples provided for Xenon, such as the notation Xe 6s[3/2]_1^o. The discussion highlights the importance of j-j coupling for labeling states in heavier rare gases and references C. E. Moore's tables and Condon & Shortley's "The Theory of Atomic Spectra" for further understanding.

PREREQUISITES
  • Understanding of atomic spectroscopy principles
  • Familiarity with electronic excitation concepts
  • Knowledge of j-j coupling in quantum mechanics
  • Access to C. E. Moore's tables and Condon & Shortley's literature
NEXT STEPS
  • Study Paschen notation in atomic spectroscopy
  • Explore j-j coupling and its applications in heavier rare gases
  • Read C. E. Moore's tables for detailed nomenclature
  • Examine Condon & Shortley's "The Theory of Atomic Spectra" for energy level discussions
USEFUL FOR

Researchers, physicists, and students in atomic spectroscopy, particularly those focusing on electronic excitation in inert gases like Xenon.

vrinda mukund
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I was trying to understand electronic excitation in Xenon. Most of the research journals are denoting different excitation levels in terms of Paschen notation, which i think, is generally used to represent excited states of inert gases. Can someone please explain how to use this paschen notation ?? Kindly help!
 
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vrinda mukund said:
I was trying to understand electronic excitation in Xenon. Most of the research journals are denoting different excitation levels in terms of Paschen notation, which i think, is generally used to represent excited states of inert gases. Can someone please explain how to use this paschen notation ?? Kindly help!
Labeling of states in the heavier rare gases often use a different notation, because j-j coupling is a better method to use to describe the states. Here, you will see things like:

Xe 6s[3/2]_1^o --> excited electron is nominally a 6s electron (j=1/2). The Xe+ p^5 ion core has j=3/2. The _1 subscript outside the bracket indicates that the j=1/2 of the excited electron and the j=3/2 of the core combine to give a state with J=1. I think that C. E. Moore discusses this nomenclature in her famous tables ... it has been a while, but that is where I believe that I learned about these.

Condon & Shortley "The Theory of Atomic Spectra" have some good discussion of the energy levels of the heavier rare gases.
 
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