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Deriving the London's equation for superconductor

 
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Dec16-12, 10:02 AM   #1
 

Deriving the London's equation for superconductor


The equation can be obtained from the fact that the "canonical momentum of the ground grstate of superconductor is zero", but where does this fact follow from.
P.S. Jackson gives a vague reference to Kittel, which I couldn't find in his Introduction_to_solid_state/Quantum_theory_of_Solids.
 
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Dec17-12, 12:54 AM   #2
 
you may start here
http://en.wikipedia.org/wiki/London_equations
v is written as p/m and usual prescription of minimal coupling is provided
p--->{p-(e/c)A}
 
Dec17-12, 01:42 AM   #3
 
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There are plenty of explanations around. Maybe the most general is due to broken symmetry arguments as expounded by Weinberg:
http://ptp.ipap.jp/link?PTPS/86/43/
 
Dec17-12, 10:02 AM   #4
 

Deriving the London's equation for superconductor


Thank you for the gem, DrDu - it is beautiful.
 
Dec18-12, 05:46 AM   #5
 
Actually, it is beautiful, but I don't understand much. Can you provide an explanation without calling for field theory?
 
Dec18-12, 09:17 AM   #6
 
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In Kittel Quantum theory of solids he discusses how a superconductor reacts to an applied transversal field of long wavelength. He finds that the wavefunction remains unchanged to lowest order. Hence the expectation of the momentum <p>=0 also does not change with A. This has already been called "rigidity of the wavefunction" by the Londons.
 
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