Why does superconductors don't radiate?

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Superconductors do not radiate electromagnetic energy due to the unique behavior of Cooper pairs, which are electron pairs that move without resistance. Unlike ordinary conductors, where electrons can lose energy through scattering and radiation, superconductors have an energy gap that prevents energy loss through scattering. Although Cooper pairs are subject to acceleration, they do not radiate because their motion is collective and maintains a constant velocity, avoiding the conditions necessary for radiation. The Meissner effect further complicates this, as it implies that photons acquire mass within superconductors, creating an energy gap for radiation. Overall, the combination of these factors explains why superconductors do not emit radiation despite the presence of accelerating charges.
  • #31
Demystifier said:
Or let me be more quantitative. According to an equation in http://en.wikipedia.org/wiki/Multipole_radiation ,
the intensity of multipole radiation is suppressed by a factor

1/(2l+1)!

For a macroscopic current, l is of the order of 10^23, so the factor above is ridiculously small. This smallness has nothing to do with superconductivity.

This argument also carries over to the quantum description of a normal conductor.
In scattering an electron has to get scattered from one side of the fermi surface with momentum k_F to the other side with -k_F. The corresponding angular momentum change is ##L=2r\hbar k_F=\hbar l## with r being the radius of the ring.
 
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  • #32
DrDu said:
The article by Greiter is dead wrong as I already laid out in another thread.

I thought you changed your mind?
 
  • #33
I had a look at the old thread
https://www.physicsforums.com/showthread.php?t=622398&highlight=Greiter
I still stand to my point that as ##|\phi\rangle=|\phi^\Lambda\rangle ## also ##\phi(x)=\langle x|\phi \rangle=\langle x|\phi^\Lambda \rangle=\phi^\Lambda ## in contrast to the assumed behaviour in first quantisation.
 
  • #34
DrDu said:
I had a look at the old thread
https://www.physicsforums.com/showthread.php?t=622398&highlight=Greiter
I still stand to my point that as ##|\phi\rangle=|\phi^\Lambda\rangle ## also ##\phi(x)=\langle x|\phi \rangle=\langle x|\phi^\Lambda \rangle=\phi^\Lambda ## in contrast to the assumed behaviour in first quantisation.

Well, let's discuss that some other time - I can't remember what it was about except that I thought you had changed your mind. Anyway, it doesn't seem controversial that the London equation is derived using a quasistatic assumption, which fits with the idea that it's a very good approximation to simply ignore any radiation - does it?
 
  • #35
I also think that the original question has been clarified:
1. For a constant macroscopic current - whether superconducting or not - we expect practically no radiation due to the homogeneity of the charge and current distributions.
2. Radiation in superconductors is supressed further by a similar mechanism as scattering, i.e.
a Cooper pair can't make an energetically favourable radiative transition to a condensate with lower velocity as this condensate is not present.
 
  • #36
DrDu said:
I also think that the original question has been clarified:
1. For a constant macroscopic current - whether superconducting or not - we expect practically no radiation due to the homogeneity of the charge and current distributions.
2. Radiation in superconductors is supressed further by a similar mechanism as scattering, i.e.
a Cooper pair can't make an energetically favourable radiative transition to a condensate with lower velocity as this condensate is not present.
As far as I am concerned, 1. is now sufficient to me.
 

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