Interaction between light and hydrogen atom

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SUMMARY

The discussion centers on the interaction between light and the hydrogen atom, specifically addressing the origin of the electric dipole moment term, denoted as ##\boldsymbol{\mu}##, in the Hamiltonian. It is established that this term arises from the electric field of light, despite a symmetric charge distribution lacking an inherent dipole moment. The electric moment for the hydrogen atom is defined as ##\boldsymbol \mu = e\mathbf r_p - e\mathbf r_e##, where the electron and proton are treated as point particles. Furthermore, when the wave function ##\psi## lacks special symmetry, the expected average value of the electric moment can be non-zero.

PREREQUISITES
  • Quantum Mechanics fundamentals
  • Understanding of Hamiltonian operators
  • Knowledge of electric dipole moments
  • Familiarity with wave functions and their properties
NEXT STEPS
  • Study the derivation of the electric dipole moment in quantum systems
  • Explore the role of the Hamiltonian in quantum mechanics
  • Investigate the implications of symmetry in quantum wave functions
  • Learn about the interaction of light with matter in quantum electrodynamics
USEFUL FOR

Physicists, quantum mechanics students, and researchers interested in atomic interactions and light-matter coupling will benefit from this discussion.

damosuz
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If a symmetric distribution of charge has no electric dipole moment, where does the [itex]\mu[/itex] term we write in the part of the hamiltonian representing interaction with light come from? We suppose it is induced by the electric field of the light?
 
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The electric moment ##\boldsymbol{\mu}## used in the Hamiltonian operator is an operator as well - for hydrogen atom, ##\boldsymbol \mu = e\mathbf r_p - e\mathbf r_e##. There is no symmetric charge distribution considered; the particles - electron and proton - are points whose possible configurations have generally non-zero electric moment.

When the ##\psi## function does not have special symmetry, the expected average value of electric moment

$$
\int \psi^* \boldsymbol{\mu} \psi\,d\tau
$$

may be non-zero as well.
 

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