Why Is the Scalar Potential Ignored in Coulomb Gauge?

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SUMMARY

The discussion centers on the treatment of scalar potential in the context of the Coulomb gauge in electromagnetism. It is established that in the Coulomb gauge, the scalar potential can be set to zero through a specific gauge transformation, allowing for simplifications in the Hamiltonian of a one-electron atom interacting with an electromagnetic field. The transformation involves adjusting the gauge function λ such that the scalar potential becomes zero while maintaining the vector potential's divergence-free condition. This approach combines principles from both the Lorenz and Coulomb gauges.

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  • Understanding of electromagnetic theory, specifically gauge transformations.
  • Familiarity with the concepts of scalar and vector potentials in electromagnetism.
  • Knowledge of the Lorenz and Coulomb gauges and their mathematical formulations.
  • Basic principles of quantum mechanics related to Hamiltonians and atomic systems.
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  • Study gauge transformations in electromagnetism, focusing on their implications for scalar and vector potentials.
  • Learn about the mathematical derivation of the Lorenz and Coulomb gauges and their applications.
  • Explore the Hamiltonian formulation of quantum mechanics for one-electron systems.
  • Investigate the physical significance of gauge invariance in electromagnetic theory.
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Students of physics, particularly those focusing on electromagnetism and quantum mechanics, as well as researchers exploring gauge theories and their applications in atomic systems.

eoghan
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Hi there,
I'm studying the interaction of one electron atom with an electromagnetic field. In every textbook the starting point is the hamiltonian of the system containing the scalar potential and the vector potential. But then the scalar potential is ignored and I don't understand why.
I've read that in the coulomb gauge I can choose the scalar potential to be 0, why??
 
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In electromagnetism, you're allowed to perform the gauge transformation

[tex]\textbf{A} \rightarrow \textbf{A}'= \textbf{A}+\nabla\lambda[/tex]

[tex]\Phi \rightarrow \Phi'= \Phi - \partial_t \lambda[/tex]

The situation you're describing is a combination of the Lorenz and Coulomb gauges. In the Lorenz gauge, you have

[tex]-\partial_t \Phi + \nabla \cdot \textbf{A} = 0[/tex]

The Lorenz gauge is only a partial gauge fixing, so you still have the freedom to do an additional gauge transformation. In particular, if you choose the gauge function λ such that

[tex]\Phi = \partial_t \lambda[/tex]

you will have, after the gauge transformation, [itex]\Phi' = 0[/itex] and [itex]\nabla\cdot\textbf{A}'=0[/itex], which is the Coulomb gauge.
 
Thank you!
 

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