Abstract:Abstract. We present a summary of our recent rigorous derivation of the celebrated Ginzburg-Landau (GL) theory, starting from the microscopic BardeenCooper-Schrieffer (BCS) model. Close to the critical temperature, GL arises as an effective theory on the macroscopic scale. The relevant scaling limit is semiclassical in nature, and semiclassical analysis, with minimal regularity assumptions, plays an important part in our proof.
“…The validity of this approximation was discussed by Gor'kov [9] and, later, by de Gennes [7] and Eilenberger [2]. In our previous work [4] (see also [5,6]) we identified a precise parameter regime where this approximation is valid and we gave the first mathematical derivation of GL theory from BCS theory with quantitative error bounds. In this paper we continue our investigation and discuss the critical temperature in the BCS model.…”
Section: Introductionmentioning
confidence: 81%
“…In [6] this was shown for D > 0, but in [8] it was remarked that the same proof works even for D ≤ 0, provided the normalization of α * is changed accordingly. …”
Section: Lemma 25 the Critical Value D C Is Uniquely Characterized mentioning
confidence: 89%
“…as h → 0. In [4] this was shown for D > 0, but in [6] it was remarked that the same proof works even for D ≤ 0, provided the normalization of α * is changed accordingly. The result (2.15) neither implies nor is implied by our Theorem 2.4 here.…”
Section: Connection To Ginzburg-landau Theorymentioning
confidence: 89%
“…Therefore, to complete the proof of Theorem 2.4 it remains to prove the following bound. 6 Lemma 6.2. Assume that an admissible Γ satisfies F T (Γ) ≤ F (0) T and define σ and ∆ by (6.14) and (6.19).…”
Abstract:We consider the Bardeen-Cooper-Schrieffer free energy functional for particles interacting via a two-body potential on a microscopic scale and in the presence of weak external fields varying on a macroscopic scale. We study the influence of the external fields on the critical temperature. We show that in the limit where the ratio between the microscopic and macroscopic scale tends to zero, the next to leading order of the critical temperature is determined by the lowest eigenvalue of the linearization of the Ginzburg-Landau equation.
“…The validity of this approximation was discussed by Gor'kov [9] and, later, by de Gennes [7] and Eilenberger [2]. In our previous work [4] (see also [5,6]) we identified a precise parameter regime where this approximation is valid and we gave the first mathematical derivation of GL theory from BCS theory with quantitative error bounds. In this paper we continue our investigation and discuss the critical temperature in the BCS model.…”
Section: Introductionmentioning
confidence: 81%
“…In [6] this was shown for D > 0, but in [8] it was remarked that the same proof works even for D ≤ 0, provided the normalization of α * is changed accordingly. …”
Section: Lemma 25 the Critical Value D C Is Uniquely Characterized mentioning
confidence: 89%
“…as h → 0. In [4] this was shown for D > 0, but in [6] it was remarked that the same proof works even for D ≤ 0, provided the normalization of α * is changed accordingly. The result (2.15) neither implies nor is implied by our Theorem 2.4 here.…”
Section: Connection To Ginzburg-landau Theorymentioning
confidence: 89%
“…Therefore, to complete the proof of Theorem 2.4 it remains to prove the following bound. 6 Lemma 6.2. Assume that an admissible Γ satisfies F T (Γ) ≤ F (0) T and define σ and ∆ by (6.14) and (6.19).…”
Abstract:We consider the Bardeen-Cooper-Schrieffer free energy functional for particles interacting via a two-body potential on a microscopic scale and in the presence of weak external fields varying on a macroscopic scale. We study the influence of the external fields on the critical temperature. We show that in the limit where the ratio between the microscopic and macroscopic scale tends to zero, the next to leading order of the critical temperature is determined by the lowest eigenvalue of the linearization of the Ginzburg-Landau equation.
“…In a remarkable work, R. Frank, Ch. Hainzl, R. Seiringer, J.P. Solovej ( [132]) have shown that, for non-dynamical magnetic fields, the nanoscopic approximation of the BdG system is given by the Ginzburg-Landau one (see also [133,134,72]).…”
We review very briefly the main mathematical structures and results in some important areas of Quantum Mechanics involving PDEs and formulate open problems. Contents 1. Preface 1 Acknowledgments 2 2. Schrödinger equation 2 3. Including photons (Nonrelativistic QED) 4 4. Effective Equations 6 5. Hartree-Fock-Bogolubov system 8 6. Bogolubov-de Gennes system 9 7. Ginzburg-Landau equations 12 8. Summary 14 9. Remarks on literature 15 Appendix A. The NR QED Hamiltonian 17 Appendix B. Hartree-Fock-Bogolubov equations 18 Appendix C. Bogolubov-de Gennes Equations: Discussion 19 References 20 1 ONEPAS and MCQM stand for Online Northeast PDE and Analysis Seminar and Mathematical Challenges in Quantum Mechanics.
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