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Analytic solution of the BCS gap equation in D dimensions (D = 1, 2, 3), at finite temperatures

机译:有限温度下D维(D = 1,2,3)的BCS间隙方程的解析解

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The Bardeen-Cooper-Schrieffer (BCS) gap equation is solved analytically in one, two and three dimensions, for temperatures close to zero and T_c. We work in the weak coupling limit, but allow the interaction width v ≡ hω_m/E_F to lie in the interval (0, ∞) Here, hω_m is the maximum energy of a force-mediating boson, and E_F denotes the Fermi energy. We obtain expressions for T_c and ΔC, the jump in the electronic specific heat across T = T_c, in the limits v 1 (the usual phonon pairing) and v > 1 (non-phononic pairing). This enables us to see how T_c scales with the mediating boson cut off. Our results predict a larger jump in the specific heat for the case v > 1, compared to v 1. We also briefly touch upon the role of a van Hove singularity in the density of states.
机译:对于温度接近零和T_c的情况,Bardeen-Cooper-Schrieffer(BCS)间隙方程可以一维,二维和三维解析地求解。我们在弱耦合极限下工作,但允许相互作用宽度v≡hω_m/ E_F在(0,∞)区间内。在此,hω_m是介力玻色子的最大能量,E_F表示费米能量。我们获得T_c和ΔC的表达式,即T = T_c上电子比热的跃迁,极限为v 1(通常的声子配对),v> 1(非声子配对)。这使我们能够看到T_c如何随着中间玻色子的截止而缩放。我们的结果预测,与v 1相比,v> 1的情况下,比热会有更大的跃迁。我们还简要介绍了范霍夫奇异性在状态密度中的作用。

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