Second quantization particle current

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Discussion Overview

The discussion revolves around the expression for charge current in the context of second quantization and its interpretation within quantum mechanics. Participants explore the implications of integrating the charge density operator and the definitions of current density versus current in various physical contexts.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Conceptual clarification

Main Points Raised

  • Some participants question why the expression for charge current includes an integral sign and whether it implies integrating out the r-dependence.
  • There is a suggestion that the expression may not represent the electromagnetic current from QED but rather the probability current for the Schrödinger equation, which typically does not involve an integral.
  • Participants discuss the concept of integrating a charge density operator over a volume and its implications for extensive physical quantities.
  • Some express confusion about taking a volume integral of current density, noting that current density is a vector and typically integrated over a surface to yield current through that surface.
  • A participant proposes a modified expression for current that includes a delta function, indicating a potential approach the author may have had in mind.
  • There is a discussion about how to calculate the total momentum of a fluid from its momentum density, which some find sensible but unfamiliar in terms of defining currents.
  • One participant notes that in curved space, the integral of a vector field is not well-defined, complicating the association of vectors to regions of space.
  • Another participant clarifies that integrating over a surface typically yields a flux, which is a scalar quantity, rather than a vector quantity.

Areas of Agreement / Disagreement

Participants express differing views on the interpretation of the integral in the charge current expression and whether it aligns with conventional definitions of current and current density. The discussion remains unresolved with multiple competing perspectives on the topic.

Contextual Notes

There are limitations regarding the definitions of current and current density, as well as the implications of integrating over volume versus surface. The discussion also touches on the complexities introduced by curved space, which may affect the interpretation of vector fields.

daudaudaudau
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Hi. I'm reading an article which writes the following

"... and the well-known expression for the charge current is"
[tex] j=-\frac{ie}{m}\int dr\psi^\dagger (r)[\nabla-ieA(r)]\psi(r)[/tex]

Why does it have an integral sign? And when you define it this way, you integrate out the r-dependence, don't you?
 
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daudaudaudau said:
Hi. I'm reading an article which writes the following

"... and the well-known expression for the charge current is"
[tex] j=-\frac{ie}{m}\int dr\psi^\dagger (r)[\nabla-ieA(r)]\psi(r)[/tex]

Why does it have an integral sign? And when you define it this way, you integrate out the r-dependence, don't you?
Strange.

I guess it's not the el.-mag current from QED which does not contain A but carries a four-vector index. Instead it seems to be the probability current for the ordinary Schrödinger equation (with a vector potential) for a particle with mass m. But even in that case there is no integral
 
I've attached a picture from the particular part of the article (Thermal transport for many-body tight-binding models by Vanderbilt and King-Smith).
 

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  • current.png
    current.png
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OK

The author decided to call the integral a current (referring to the integrand as the current density).
 
But still he is taking a volume integral of a charge density operator. What is this?
 
daudaudaudau said:
But still he is taking a volume integral of a charge density operator. What is this?
For any extensive physical quantity Q, you can say that it is equal to the volume integral of the DENSITY of Q.
 
But when would you ever take the volume integral of the current density? The current density is a vector, and it has units A/m^2. What you would normally do is integrate it over a surface to get the current through the surface.
 
Probably he had something like
[tex] j(r')=-\frac{ie}{2m}\int dr\psi^\dagger (r) \{\nabla_{r'}-ieA(r'),\delta(r-r')\}\psi(r)[/tex]
in mind.
 
daudaudaudau said:
But when would you ever take the volume integral of the current density? The current density is a vector, and it has units A/m^2. What you would normally do is integrate it over a surface to get the current through the surface.
Assume that you have a fluid, each part of which has some momentum density. How would you calculate the momentum of the fluid as a whole?
 
  • #10
Demystifier said:
Assume that you have a fluid, each part of which has some momentum density. How would you calculate the momentum of the fluid as a whole?

Yes that sounds sensible, I have just never heard of currents defined in this way before. What should I google to find out more about this?
 
  • #11
daudaudaudau said:
Yes that sounds sensible, I have just never heard of currents defined in this way before. What should I google to find out more about this?
I think you are right that such global vector quantities are usually not CALLED currents, so googling probably would not help.

In fact, in curved space the integral of a vector field is not even well defined. In other words, in curved space you can associate a vector to a point, but you cannot associate a vector to a whole region of space.
 
  • #12
daudaudaudau said:
What you would normally do is integrate it over a surface to get the current through the surface.
Actually, normally you would obtain a FLUX, which is a scalar, not a vector. See also my post above.
 

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