Can Magnetism Alter Quantum Phase in Superconductors?

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SUMMARY

The discussion centers on the quantization of magnetic flux in superconducting rings, specifically addressing the relationship between the phase of the order parameter and the quantized flux. The integral of the gradient of the phase, \(\oint\nabla\theta dl\), equates to \(2\pi n\) due to the requirement for the wavefunction to be single-valued, leading to the conclusion that the quantized flux is \(\Phi_s = nh/e^*\). Participants also explore experimental methods to alter the phase of the supercurrent wavefunction, suggesting the introduction of magnetic flux as a viable approach.

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  • Understanding of superconductivity principles, particularly Cooper pairs and their dynamics.
  • Familiarity with quantum mechanics, specifically wavefunctions and phase factors.
  • Knowledge of Stokes' theorem and its application in physics.
  • Basic concepts of magnetic flux and its role in superconducting circuits.
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sniffer
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in deriving quantization of flux in superconductor ring, the momentum of cooper pair p:
p=\hbar\nabla\theta=e^*(\Lambda J_s + A)
then integrate around the ring,
\hbar\oint\nabla\theta dl=e^*\oint(\Lambda J_s + A)dl
using stoke's theorem and integrate sufficiently deep in the ring where current density is very small, the RHS becomes
RHS=e^*\Phi_s
and the left hand side,becomes hn where n is integer.
So the quantized flux is
\Phi_s=nh/e^*
e star is the effective cooper pair charge which is -2e.

i got confused here,why the left hand side integral becomes hn?

The argument used by the book (Van Duzer, superconductivity page 116) is that because theta is unique or differ by a multiple of 2 Pi at each point, so the integral
\oint\nabla\theta dl=2\pi n
why?? where does n come from? theta is a scalar function of r.
please help.

thanks.
 
Last edited:
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\theta is the phase of the order parameter \psi = |\psi|e^{i \theta}. Since \psi must be single valued at some specific angular position \phi + 2k \pi on the ring, we need, \psi(\phi ) = \psi(\phi + 2m \pi ), or we need e^{i \theta ( \phi )} = e^{i \theta ( \phi + 2m \pi)}, for all m. For the phase factor to remain unchanged over integral number of traversals of the loop, the phase \theta must itself change by only an integer multiple of 2 \pi (since e^{2in \pi} = 1).

So
\theta ( \phi + 2m \pi ) = \theta ( \phi) + 2n \pi.

In other words
\hbar\oint\nabla\theta dl = \hbar \Delta\theta = \hbar (\theta ( \phi + 2 \pi ) - \theta ( \phi)) = 2 \pi n \hbar = nh
 
Last edited:
Good answer, Gokul.

In your opinion, from an experimental point of view, what would be a simple method to effect a change in the phase of the wavefunction of the supercurrent while remaining below T(c)?

Creator :biggrin:
 
Last edited:
change the radius of the ring.
 
Creator said:
Good answer, Gokul.

In your opinion, from an experimental point of view, what would be a simple method to effect a change in the phase of the wavefunction of the supercurrent while remaining below T(c)?

Creator :biggrin:

Have a magnetic flux through the loop. That, after all, is how a SQUID works.

Zz.
 
sniffer said:
change the radius of the ring.

True, in theory; but by what method are you going to change the length of a brittle superconducting wire while it is in the superconducting state?
:biggrin:
 
ZapperZ said:
Have a magnetic flux through the loop. That, after all, is how a SQUID works.

Zz.

Of course; externally applying B thru the loop. I should be more specific. I guess I am referring to a non-electromagnetic method of altering the quantum phase.

Creator
 
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