Selection Rules for a Diatomic Molecule?

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SUMMARY

The discussion centers on the selection rules for electronic transitions in diatomic molecules, specifically addressing the confusion surrounding the rules ΔΛ=0 and ΔΛ=0, ±1 as outlined in Bransden and Joachain's "Physics of Atoms and Molecules". The correct interpretation is that ΔΛ=0, ±1 applies in general cases, while ΔΛ=0 is a specific scenario. The participants emphasize the need to differentiate between cases where one or both λ values are zero when describing transitions between electronic states. Additionally, classic references such as G. Herzberg's "Molecular Spectra and Molecular Structure" and Townes and Scawlow's "Microwave Spectroscopy" are recommended for further clarity on the topic.

PREREQUISITES
  • Understanding of diatomic molecular structure
  • Familiarity with quantum mechanics principles
  • Knowledge of selection rules in spectroscopy
  • Access to Bransden and Joachain's "Physics of Atoms and Molecules" (2nd edition)
NEXT STEPS
  • Study G. Herzberg's "Molecular Spectra and Molecular Structure" for foundational concepts
  • Review C. H. Townes and A. L. Scawlow's "Microwave Spectroscopy" for advanced insights
  • Explore the implications of ΔK selection rules in molecular transitions
  • Investigate the role of rotational spectra in understanding electronic transitions
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Students and researchers in molecular physics, chemists specializing in spectroscopy, and educators teaching quantum mechanics and molecular structure concepts.

Sebacide
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Hello!
I have a question about selection rules and electronic transitions of a diatomic molecule: I can't find a good explanation about that, and there's so much confusion about the right rules to use.
I studied that on Bransden-Joachain's "Physics of atoms and molecules", but there (to whom have the book, paragraphs 11.1 and 11.3 of 2nd edition) is said that diatomic molecules are forced to have a transition with ΔΛ=0, and, some pages on, that there is a rule ΔΛ=0,+-1; so, which is the right one?
Surely they are referred to different situations, but it is not explained very clearly.
Thanks for the answers!
 
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I don't really understand what Bransden and Joachain are saying in 11.1. They are discussing pure rotational spectra, so I don't see why they invoke ##\Delta \Lambda##.

In any case, 11.3 is correct and ##\Delta \Lambda = 0, \pm 1##.
 
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Hi, thank you for your help: I thought the same, but during class it was mentioned the ##\Delta \Lambda=0## only.
So, if I have to describe the possible transition between two fixed electonic states, I have to separate the case in which one of the two lamdas is not zero and the one they are zero?
 
Sebacide said:
Hi, thank you for your help: I thought the same, but during class it was mentioned the ##\Delta \Lambda=0## only.
So, if I have to describe the possible transition between two fixed electonic states, I have to separate the case in which one of the two lamdas is not zero and the one they are zero?
The selection rules on ##\Delta K## is not the same for ##\Lambda = 0 \leftrightarrow \Lambda = 0## than for ##\Lambda \neq 0 \leftrightarrow \Lambda \neq 0##
 
Sebacide said:
I have a question about selection rules and electronic transitions of a diatomic molecule: I can't find a good explanation about that, and there's so much confusion about the right rules to use.
The following books provide definitive discussions of the selection rules:

1. G. Herzberg, "Molecular Spectra and Molecular Structure. Volume I: Spectra of Diatomic Molecules. Second Edition" D. Van Nostrand, 1950.

2. C. H. Townes and A. L. Scawlow, "Microwave Spectroscopy", McGraw Hill, 1955.

While not new books, they are classic discussions of the fundamental concepts.
 

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