How Is Non s-Wave Superconductivity Gap Parameter Chosen?

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SUMMARY

The discussion centers on the selection of the non s-wave superconductivity gap parameter, specifically the d-wave gap represented by the equation \Delta_0 = [ \cos (k_x a) - \cos (k_y a)]. It highlights the use of group theory and crystal lattice symmetry to calculate the gap parameter. The t-J method, utilizing mean-field approximation, is mentioned as a controversial approach that may yield d-wave symmetry. Additionally, the influence of atomic orbitals, particularly the d-orbitals of transition metals like Cu in CuO planes, is emphasized as a key factor in determining the effective electron-electron interaction.

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  • Understanding of BCS theory and its assumptions regarding electron interactions.
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  • Knowledge of superconductivity types, particularly d-wave and p-wave symmetries.
  • Experience with the t-J model and mean-field approximations in condensed matter physics.
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In BCS you make the assumption that the effective electron-electron interaction is constant within a small shell around the fermi surface and zero otherwise. From this you get a constant spherical gap.

In non s-wave SC there is a specific form for the gap ie, \Delta_0 = [ \cos (k_x a) - \cos (k_y a)]. I know that you can calculate the gap parameter using group theory and the underlying symmetry of the crystal lattice. But is there a way to choose an arbitary form for k \cdot k^\prime, self consistently solve the gap equation and arrive at a d-wave gap or any other non s-wave gap?

How do you choose the effective electron-electron interaction? Is it based on the atomic orbitals that are believed to be responsible for SC? I've done a few searches and all I find is a assumption for the form of the gap. Thanks
 
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nbo10 said:
In BCS you make the assumption that the effective electron-electron interaction is constant within a small shell around the fermi surface and zero otherwise. From this you get a constant spherical gap.

In non s-wave SC there is a specific form for the gap ie, \Delta_0 = [ \cos (k_x a) - \cos (k_y a)]. I know that you can calculate the gap parameter using group theory and the underlying symmetry of the crystal lattice. But is there a way to choose an arbitary form for k \cdot k^\prime, self consistently solve the gap equation and arrive at a d-wave gap or any other non s-wave gap?

How do you choose the effective electron-electron interaction? Is it based on the atomic orbitals that are believed to be responsible for SC? I've done a few searches and all I find is a assumption for the form of the gap. Thanks

This isn't an easy question to answer because this is still something being worked on. Something like the t-J method using mean-field approximation can drop the d-wave symmetry onto your lap (this assertion is still controversial). In many instances, the symmetry is inserted by hand because that is the product of experimental observation. There's a persuasive reason why this is having that d-wave symmetry - the valence shell of the Cu in the CuO plane where superconductivity is thought to reside. The transition metals have d-orbitals valence shell.

Note that for the Ruthenates, you have a p-wave symmetry for the pair.

Zz.
 

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