@article{22290, abstract = {We introduce a multi-band BCS free energy functional and prove that for a multi-band superconductor the effect of inter-band coupling can only increase the critical temperature, irrespective of its attractive or repulsive nature and its strength. Further, for weak coupling and weaker inter-band coupling, we prove that the dependence of the increase in critical temperature on the inter-band coupling is (1) linear, if there are two or more equally strongly superconducting bands, or (2) quadratic, if there is only one dominating band.}, author = {Henheik, Sven Joscha and Langmann, Edwin and Lauritsen, Asbjørn Bækgaard}, issn = {1424-0661}, journal = {Annales Henri Poincaré}, publisher = {Springer Nature}, title = {{Multi-band superconductors have enhanced critical temperatures}}, doi = {10.1007/s00023-026-01706-y}, year = {2026}, } @article{12232, abstract = {We derive a precise asymptotic formula for the density of the small singular values of the real Ginibre matrix ensemble shifted by a complex parameter z as the dimension tends to infinity. For z away from the real axis the formula coincides with that for the complex Ginibre ensemble we derived earlier in Cipolloni et al. (Prob Math Phys 1:101–146, 2020). On the level of the one-point function of the low lying singular values we thus confirm the transition from real to complex Ginibre ensembles as the shift parameter z becomes genuinely complex; the analogous phenomenon has been well known for eigenvalues. We use the superbosonization formula (Littelmann et al. in Comm Math Phys 283:343–395, 2008) in a regime where the main contribution comes from a three dimensional saddle manifold.}, author = {Cipolloni, Giorgio and Erdös, László and Schröder, Dominik J}, issn = {1424-0661}, journal = {Annales Henri Poincaré}, keywords = {Mathematical Physics, Nuclear and High Energy Physics, Statistical and Nonlinear Physics}, number = {11}, pages = {3981--4002}, publisher = {Springer Nature}, title = {{Density of small singular values of the shifted real Ginibre ensemble}}, doi = {10.1007/s00023-022-01188-8}, volume = {23}, year = {2022}, } @article{9912, abstract = {In the customary random matrix model for transport in quantum dots with M internal degrees of freedom coupled to a chaotic environment via 𝑁≪𝑀 channels, the density 𝜌 of transmission eigenvalues is computed from a specific invariant ensemble for which explicit formula for the joint probability density of all eigenvalues is available. We revisit this problem in the large N regime allowing for (i) arbitrary ratio 𝜙:=𝑁/𝑀≤1; and (ii) general distributions for the matrix elements of the Hamiltonian of the quantum dot. In the limit 𝜙→0, we recover the formula for the density 𝜌 that Beenakker (Rev Mod Phys 69:731–808, 1997) has derived for a special matrix ensemble. We also prove that the inverse square root singularity of the density at zero and full transmission in Beenakker’s formula persists for any 𝜙<1 but in the borderline case 𝜙=1 an anomalous 𝜆−2/3 singularity arises at zero. To access this level of generality, we develop the theory of global and local laws on the spectral density of a large class of noncommutative rational expressions in large random matrices with i.i.d. entries.}, author = {Erdös, László and Krüger, Torben H and Nemish, Yuriy}, issn = {1424-0661}, journal = {Annales Henri Poincaré }, pages = {4205–4269}, publisher = {Springer Nature}, title = {{Scattering in quantum dots via noncommutative rational functions}}, doi = {10.1007/s00023-021-01085-6}, volume = {22}, year = {2021}, } @article{6788, abstract = {We consider the Nelson model with ultraviolet cutoff, which describes the interaction between non-relativistic particles and a positive or zero mass quantized scalar field. We take the non-relativistic particles to obey Fermi statistics and discuss the time evolution in a mean-field limit of many fermions. In this case, the limit is known to be also a semiclassical limit. We prove convergence in terms of reduced density matrices of the many-body state to a tensor product of a Slater determinant with semiclassical structure and a coherent state, which evolve according to a fermionic version of the Schrödinger–Klein–Gordon equations.}, author = {Leopold, Nikolai K and Petrat, Sören P}, issn = {1424-0661}, journal = {Annales Henri Poincare}, number = {10}, pages = {3471–3508}, publisher = {Springer Nature}, title = {{Mean-field dynamics for the Nelson model with fermions}}, doi = {10.1007/s00023-019-00828-w}, volume = {20}, year = {2019}, } @article{2743, abstract = {We consider the supersymmetric quantum mechanical system which is obtained by dimensionally reducing d = 6, N = 1 supersymmetric gauge theory with gauge group U(1) and a single charged hypermultiplet. Using the deformation method and ideas introduced by Porrati and Rozenberg [1], we present a detailed proof of the existence of a normalizable ground state for this system.}, author = {Erdös, László and Hasler, David and Solovej, Jan}, issn = {1424-0661}, journal = {Annales Henri Poincare}, number = {2}, pages = {247 -- 267}, publisher = {Birkhäuser}, title = {{Existence of the D0-D4 bound state: A detailed proof}}, doi = {10.1007/s00023-005-0205-0}, volume = {6}, year = {2005}, } @article{2741, abstract = {The Pauli operator describes the energy of a nonrelativistic quantum particle with spin 1/2 in a magnetic field and an external potential. A new Lieb-Thirring type inequality on the sum of the negative eigenvalues is presented. The main feature compared to earlier results is that in the large field regime the present estimate grows with the optimal (first) power of the strength of the magnetic field. As a byproduct of the method, we also obtain an optimal upper bound on the pointwise density of zero energy eigenfunctions of the Dirac operator. The main technical tools are: (i) a new localization scheme for the square of the resolvent of a general class of second order elliptic operators; (ii) a geometric construction of a Dirac operator with a constant magnetic field that approximates the original Dirac operator in a tubular neighborhood of a fixed field line. The errors may depend on the regularity of the magnetic field but they are uniform in the field strength.}, author = {Erdös, László and Solovej, Jan}, issn = {1424-0661}, journal = {Annales Henri Poincare}, number = {4}, pages = {671 -- 741}, publisher = {Birkhäuser}, title = {{Uniform Lieb-Thirring inequality for the three-dimensional Pauli operator with a strong non-homogeneous magnetic field}}, doi = {10.1007/s00023-004-0180-x}, volume = {5}, year = {2004}, }