Continuity equation for Schrodinger equation with minimal coupling

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Discussion Overview

The discussion revolves around the continuity equation associated with the Schrödinger equation when minimally coupled to an electromagnetic field, specifically in the context of gauge choices. Participants explore the existence of a generalized continuity equation that does not rely on the Coulomb gauge, examining implications for gauge invariance and the form of the equation.

Discussion Character

  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant presents the continuity equation in the context of the Schrödinger equation with minimal coupling, questioning the existence of a generalized form without fixing the Coulomb gauge.
  • Another participant asserts that the continuity equation is gauge-invariant, suggesting it ensures probability conservation.
  • A different viewpoint emphasizes that gauge invariance applies only under gauge transformations compatible with the Coulomb gauge constraint, raising the question of an equation that does not require this constraint.
  • One participant proposes starting from the Schrödinger equation with arbitrary potentials to derive the equation for the probability density ρ.
  • Another participant expresses concern that the derived equation for ρ may not maintain the standard form of a temporal derivative plus the gradient of a current.
  • A later reply clarifies that it should be referred to as the divergence of current rather than just a gradient.

Areas of Agreement / Disagreement

Participants express differing views on the implications of gauge invariance and the form of the continuity equation, indicating that multiple competing perspectives remain without a consensus.

Contextual Notes

The discussion highlights limitations related to gauge choices and the potential complexity of the equations derived from arbitrary potentials, which may not conform to the expected forms.

nembokid
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The Schrödinger equation with the minimal coupling to the Electromagnetic field, in the Coulomb gauge [tex]\nabla \cdot A[/tex], has a continuity equation [tex]\partial_t \rho = \nabla \cdot j[/tex] where [tex]j \propto Re[p^* D p][/tex] (D is the covariant gradient [tex]D= \nabla + iA[/tex].

My question is: is there any continuity equation which generalized the preceding one, without having to fix the Coulomb gauge? I think that, being the Schrödinger equation nonrelativistic, a choice of a noncovariant gauge is necessary, but maybe some ugly-to-see equation still exists.

thank you
 
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It seems to me that this continuity equation is gauge-invariant. It means the probability conservation.
 
Last edited:
It's gauge invariant as long as you perform gauge transformations compatible with the Coulomb gauge constraint (which does not fix completely the gauge, as is well known). But what about an equation which does not require this constraint?
 
It is the same. Start from the Schroedinger equation with an arbitrary A and φ and find the equation for ρ.
 
But this equation for [tex]\rho[/tex] has no longer the form of a temporal derivative plus the gradient of a current (at least, I can't see how to put it in this form).
 
It should not be a gradient but divergence of current: divj.
 

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