Molecular States, Symmetry and Allowed Transitions

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SUMMARY

The discussion centers on the conditions for allowed electric dipole transitions between molecular states, specifically addressing the transition dipole moment \langle \psi_{f}|\textbf{μ}\left|\psi_{i} \right \rangle. For a transition to have a non-zero probability, the irreducible symmetry representations of the initial and final states must include the totally symmetric irreducible representation. The query raised pertains to whether the initial and final states refer to the overall molecular states or the individual single electron states, emphasizing the importance of considering the many-electron state in diatomic hydrogen transitions, such as \sigma_{g} \rightarrow \sigma_{u.

PREREQUISITES
  • Understanding of electric dipole transitions in quantum mechanics
  • Familiarity with irreducible representations in group theory
  • Knowledge of molecular orbital theory, particularly in diatomic molecules
  • Basic concepts of many-electron systems in quantum chemistry
NEXT STEPS
  • Study the role of irreducible representations in molecular symmetry
  • Explore the concept of transition dipole moments in quantum mechanics
  • Learn about many-electron wave functions and their implications for molecular transitions
  • Investigate specific examples of electric dipole transitions in diatomic molecules
USEFUL FOR

Quantum chemists, molecular physicists, and students studying molecular transitions and symmetry in quantum mechanics will benefit from this discussion.

tomothy
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I have a question about allowed transitions and molecular states. For an electric dipole transition between two states (say molecular or atomic) to have a non-zero probability of occurring, the transition dipole moment \langle \psi_{f}|\textbf{μ}\left|\psi_{i} \right \rangle must be non-zero. This can be determined by considering the irreducible symmetry representations to which each state/operator belongs i.e. \Gamma ( \psi_{f} ) \otimes \Gamma \left(x,y,z \right) \otimes \Gamma \left(\psi_{i}\right) must contain the totally symmetric irreducible representation at least once.

My question is, are the initial states and final states to be considered the overall molecular states or the individual single electron states? e.g. in diatomic hydrogen, for a \sigma_{g} \rightarrow \sigma_{u} transition, are the initial and final states the electron states of the electron being excited or the overall initial and final molecular states (i.e. of both electrons)?
 
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It is the many-electron state that must be considered.
 

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