@article{14854,
  abstract     = {
Abstract
We study the spectrum of the Fröhlich Hamiltonian for the polaron at fixed total momentum. We prove the existence of excited eigenvalues between the ground state energy and the essential spectrum at strong coupling. In fact, our main result shows that the number of excited energy bands diverges in the strong coupling limit. To prove this we derive upper bounds for the min-max values of the corresponding fiber Hamiltonians and compare them with the bottom of the essential spectrum, a lower bound on which was recently obtained by Brooks and Seiringer (Comm. Math. Phys. 404:1 (2023), 287–337). The upper bounds are given in terms of the ground state energy band shifted by momentum-independent excitation energies determined by an effective Hamiltonian of Bogoliubov type.},
  author       = {Mitrouskas, David Johannes and Seiringer, Robert},
  issn         = {2578-5885},
  journal      = {Pure and Applied Analysis},
  keywords     = {General Medicine},
  number       = {4},
  pages        = {973--1008},
  publisher    = {Mathematical Sciences Publishers},
  title        = {{Ubiquity of bound states for the strongly coupled polaron}},
  doi          = {10.2140/paa.2023.5.973},
  volume       = {5},
  year         = {2023},
}

@article{14889,
  abstract     = {We consider the Fröhlich Hamiltonian with large coupling constant α. For initial data of Pekar product form with coherent phonon field and with the electron minimizing the corresponding energy, we provide a norm approximation of the evolution, valid up to times of order α2. The approximation is given in terms of a Pekar product state, evolved through the Landau-Pekar equations, corrected by a Bogoliubov dynamics taking quantum fluctuations into account. This allows us to show that the Landau-Pekar equations approximately describe the evolution of the electron- and one-phonon reduced density matrices under the Fröhlich dynamics up to times of order α2.},
  author       = {Leopold, Nikolai K and Mitrouskas, David Johannes and Rademacher, Simone Anna Elvira and Schlein, Benjamin and Seiringer, Robert},
  issn         = {2578-5885},
  journal      = {Pure and Applied Analysis},
  number       = {4},
  pages        = {653--676},
  publisher    = {Mathematical Sciences Publishers},
  title        = {{Landau–Pekar equations and quantum fluctuations for the dynamics of a strongly coupled polaron}},
  doi          = {10.2140/paa.2021.3.653},
  volume       = {3},
  year         = {2021},
}

@article{14890,
  abstract     = {We consider a system of N interacting bosons in the mean-field scaling regime and construct corrections to the Bogoliubov dynamics that approximate the true N-body dynamics in norm to arbitrary precision. The N-independent corrections are given in terms of the solutions of the Bogoliubov and Hartree equations and satisfy a generalized form of Wick's theorem. We determine the n-point correlation functions of the excitations around the condensate, as well as the reduced densities of the N-body system, to arbitrary accuracy, given only the knowledge of the two-point functions of a quasi-free state and the solution of the Hartree equation. In this way, the complex problem of computing all n-point correlation functions for an interacting N-body system is essentially reduced to the problem of solving the Hartree equation and the PDEs for the Bogoliubov two-point functions.},
  author       = {Bossmann, Lea and Petrat, Sören P and Pickl, Peter and Soffer, Avy},
  issn         = {2578-5885},
  journal      = {Pure and Applied Analysis},
  number       = {4},
  pages        = {677--726},
  publisher    = {Mathematical Sciences Publishers},
  title        = {{Beyond Bogoliubov dynamics}},
  doi          = {10.2140/paa.2021.3.677},
  volume       = {3},
  year         = {2021},
}

@article{14891,
  abstract     = {We give the first mathematically rigorous justification of the local density approximation in density functional theory. We provide a quantitative estimate on the difference between the grand-canonical Levy–Lieb energy of a given density (the lowest possible energy of all quantum states having this density) and the integral over the uniform electron gas energy of this density. The error involves gradient terms and justifies the use of the local density approximation in the situation where the density is very flat on sufficiently large regions in space.},
  author       = {Lewin, Mathieu and Lieb, Elliott H. and Seiringer, Robert},
  issn         = {2578-5885},
  journal      = {Pure and Applied Analysis},
  number       = {1},
  pages        = {35--73},
  publisher    = {Mathematical Sciences Publishers},
  title        = {{ The local density approximation in density functional theory}},
  doi          = {10.2140/paa.2020.2.35},
  volume       = {2},
  year         = {2020},
}

@article{6186,
  abstract     = {We prove that the local eigenvalue statistics of real symmetric Wigner-type
matrices near the cusp points of the eigenvalue density are universal. Together
with the companion paper [arXiv:1809.03971], which proves the same result for
the complex Hermitian symmetry class, this completes the last remaining case of
the Wigner-Dyson-Mehta universality conjecture after bulk and edge
universalities have been established in the last years. We extend the recent
Dyson Brownian motion analysis at the edge [arXiv:1712.03881] to the cusp
regime using the optimal local law from [arXiv:1809.03971] and the accurate
local shape analysis of the density from [arXiv:1506.05095, arXiv:1804.07752].
We also present a PDE-based method to improve the estimate on eigenvalue
rigidity via the maximum principle of the heat flow related to the Dyson
Brownian motion.},
  author       = {Cipolloni, Giorgio and Erdös, László and Krüger, Torben H and Schröder, Dominik J},
  issn         = {2578-5885},
  journal      = {Pure and Applied Analysis },
  number       = {4},
  pages        = {615–707},
  publisher    = {MSP},
  title        = {{Cusp universality for random matrices, II: The real symmetric case}},
  doi          = {10.2140/paa.2019.1.615},
  volume       = {1},
  year         = {2019},
}

