An operator-theoretical proof for the second-order phase transition in the BCS-Bogoliubov model of superconductivity (final version)
arXiv:1712.09295 · doi:10.2206/kyushujm.74.177
Abstract
We show that the transition from a normal conducting state to a superconducting state is a second-order phase transition in the BCS-Bogoliubov model of superconductivity from the viewpoint of operator theory. Here we have no magnetic field. Moreover we obtain the exact and explicit expression for the gap in the specific heat at constant volume at the transition temperature. To this end, we have to differentiate the thermodynamic potential with respect to the temperature two times. Since there is the solution to the BCS-Bogoliubov gap equation in the form of the thermodynamic potential, we have to differentiate the solution with respect to the temperature two times. Therefore, we need to show that the solution to the BCS-Bogoliubov gap equation is differentiable with respect to the temperature two times as well as its existence and uniqueness. We carry out its proof on the basis of fixed point theorems.
Kyushu Journal of Mathematics, in press. arXiv admin note: substantial text overlap with arXiv:1607.00090, arXiv:1609.07224
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Cited by in corpus (5)
- Smoothness and monotone decreasingness of the solution to the BCS-Bogoliubov gap equation for superconductivity
- An operator-theoretical study of the specific heat and the critical magnetic field in the BCS-Bogoliubov model of superconductivity
- Another operator-theoretical proof for the second-order phase transition in the BCS-Bogoliubov model of superconductivity
- An operator-theoretical study on the BCS-Bogoliubov model of superconductivity near absolute zero temperature
- The BCS-Bogoliubov gap equation with external magnetic field and the first-order phase transition