Apr. 20: Hartree-Fock-Bogoliubov, BCS
Apr. 20: Hartree-Fock-Bogoliubov, BCS
Apr. 20: Hartree-Fock-Bogoliubov, BCS
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(2) Analytical solution for simple model.<br />
Assume constant interaction G, constant gap ∆, and constant density<br />
of states ρ, and restrict summation to the vicinity δ of the Fermi<br />
surface. Gap equation:<br />
1 = G 2<br />
µ+δ ∫<br />
µ−δ<br />
For weak pairing Gρ ≪ 1 one finds<br />
ρ(ε)<br />
dε√ (ε − µ)2 + ∆ = Gρ arsinh δ 2 ∆<br />
⎛<br />
∆<br />
δ ∝ exp ⎜<br />
−1<br />
⎝<br />
|G|ρ<br />
Gap is nonperturbative in interaction G!<br />
The particle number variance is<br />
(∆N) 2 ≈ 2ρ∆ atan δ ⎧<br />
⎪⎨<br />
∆ = πρ∆ for weak pairing ∆ ≪ δ,<br />
⎪ ⎩ 2ρδ for strong pairing.<br />
⎞<br />
⎟<br />
⎠