@article{13271,
  abstract     = {In this paper, we prove the convexity of trace functionals (A,B,C)↦Tr|BpACq|s,
for parameters (p, q, s) that are best possible, where B and C are any n-by-n positive-definite matrices, and A is any n-by-n matrix. We also obtain the monotonicity versions of trace functionals of this type. As applications, we extend some results in Carlen et al. (Linear Algebra Appl 490:174–185, 2016), Hiai and Petz (Publ Res Inst Math Sci 48(3):525-542, 2012) and resolve a conjecture in Al-Rashed and Zegarliński (Infin Dimens Anal Quantum Probab Relat Top 17(4):1450029, 2014) in the matrix setting. Other conjectures in Al-Rashed and Zegarliński (Infin Dimens Anal Quantum Probab Relat Top 17(4):1450029, 2014) will also be discussed. We also show that some related trace functionals are not concave in general. Such concavity results were expected to hold in different problems.},
  author       = {Zhang, Haonan},
  issn         = {1424-0637},
  journal      = {Annales Henri Poincare},
  publisher    = {Springer Nature},
  title        = {{Some convexity and monotonicity results of trace functionals}},
  doi          = {10.1007/s00023-023-01345-7},
  year         = {2023},
}

@article{12087,
  abstract     = {Following up on the recent work on lower Ricci curvature bounds for quantum systems, we introduce two noncommutative versions of curvature-dimension bounds for symmetric quantum Markov semigroups over matrix algebras. Under suitable such curvature-dimension conditions, we prove a family of dimension-dependent functional inequalities, a version of the Bonnet–Myers theorem and concavity of entropy power in the noncommutative setting. We also provide examples satisfying certain curvature-dimension conditions, including Schur multipliers over matrix algebras, Herz–Schur multipliers over group algebras and generalized depolarizing semigroups.},
  author       = {Wirth, Melchior and Zhang, Haonan},
  issn         = {1424-0637},
  journal      = {Annales Henri Poincare},
  pages        = {717--750},
  publisher    = {Springer Nature},
  title        = {{Curvature-dimension conditions for symmetric quantum Markov semigroups}},
  doi          = {10.1007/s00023-022-01220-x},
  volume       = {24},
  year         = {2023},
}

@article{12183,
  abstract     = {We consider a gas of n bosonic particles confined in a box [−ℓ/2,ℓ/2]3 with Neumann boundary conditions. We prove Bose–Einstein condensation in the Gross–Pitaevskii regime, with an optimal bound on the condensate depletion. Moreover, our lower bound for the ground state energy in a small box [−ℓ/2,ℓ/2]3 implies (via Neumann bracketing) a lower bound for the ground state energy of N bosons in a large box [−L/2,L/2]3 with density ρ=N/L3 in the thermodynamic limit.},
  author       = {Boccato, Chiara and Seiringer, Robert},
  issn         = {1424-0637},
  journal      = {Annales Henri Poincare},
  pages        = {1505--1560},
  publisher    = {Springer Nature},
  title        = {{The Bose Gas in a box with Neumann boundary conditions}},
  doi          = {10.1007/s00023-022-01252-3},
  volume       = {24},
  year         = {2023},
}

@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{9351,
  abstract     = {We consider the many-body quantum evolution of a factorized initial data, in the mean-field regime. We show that fluctuations around the limiting Hartree dynamics satisfy large deviation estimates that are consistent with central limit theorems that have been established in the last years. },
  author       = {Kirkpatrick, Kay and Rademacher, Simone Anna Elvira and Schlein, Benjamin},
  issn         = {1424-0637},
  journal      = {Annales Henri Poincare},
  pages        = {2595--2618},
  publisher    = {Springer Nature},
  title        = {{A large deviation principle in many-body quantum dynamics}},
  doi          = {10.1007/s00023-021-01044-1},
  volume       = {22},
  year         = {2021},
}

@article{10537,
  abstract     = {We consider the quantum many-body evolution of a homogeneous Fermi gas in three dimensions in the coupled semiclassical and mean-field scaling regime. We study a class of initial data describing collective particle–hole pair excitations on the Fermi ball. Using a rigorous version of approximate bosonization, we prove that the many-body evolution can be approximated in Fock space norm by a quasi-free bosonic evolution of the collective particle–hole excitations.},
  author       = {Benedikter, Niels P and Nam, Phan Thành and Porta, Marcello and Schlein, Benjamin and Seiringer, Robert},
  issn         = {1424-0637},
  journal      = {Annales Henri Poincaré},
  publisher    = {Springer Nature},
  title        = {{Bosonization of fermionic many-body dynamics}},
  doi          = {10.1007/s00023-021-01136-y},
  year         = {2021},
}

@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{8705,
  abstract     = {We consider the quantum mechanical many-body problem of a single impurity particle immersed in a weakly interacting Bose gas. The impurity interacts with the bosons via a two-body potential. We study the Hamiltonian of this system in the mean-field limit and rigorously show that, at low energies, the problem is well described by the Fröhlich polaron model.},
  author       = {Mysliwy, Krzysztof and Seiringer, Robert},
  issn         = {1424-0637},
  journal      = {Annales Henri Poincare},
  number       = {12},
  pages        = {4003--4025},
  publisher    = {Springer Nature},
  title        = {{Microscopic derivation of the Fröhlich Hamiltonian for the Bose polaron in the mean-field limit}},
  doi          = {10.1007/s00023-020-00969-3},
  volume       = {21},
  year         = {2020},
}

@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{556,
  abstract     = {We investigate the free boundary Schur process, a variant of the Schur process introduced by Okounkov and Reshetikhin, where we allow the first and the last partitions to be arbitrary (instead of empty in the original setting). The pfaffian Schur process, previously studied by several authors, is recovered when just one of the boundary partitions is left free. We compute the correlation functions of the process in all generality via the free fermion formalism, which we extend with the thorough treatment of “free boundary states.” For the case of one free boundary, our approach yields a new proof that the process is pfaffian. For the case of two free boundaries, we find that the process is not pfaffian, but a closely related process is. We also study three different applications of the Schur process with one free boundary: fluctuations of symmetrized last passage percolation models, limit shapes and processes for symmetric plane partitions and for plane overpartitions.},
  author       = {Betea, Dan and Bouttier, Jeremie and Nejjar, Peter and Vuletic, Mirjana},
  issn         = {1424-0637},
  journal      = {Annales Henri Poincare},
  number       = {12},
  pages        = {3663--3742},
  publisher    = {Springer Nature},
  title        = {{The free boundary Schur process and applications I}},
  doi          = {10.1007/s00023-018-0723-1},
  volume       = {19},
  year         = {2018},
}

@article{5813,
  abstract     = {We consider homogeneous Bose gas in a large cubic box with periodic boundary conditions, at zero temperature. We analyze its excitation spectrum in a certain kind of a mean-field infinite-volume limit. We prove that under appropriate conditions the excitation spectrum has the form predicted by the Bogoliubov approximation. Our result can be viewed as an extension of the result of Seiringer (Commun. Math. Phys.306:565–578, 2011) to large volumes.},
  author       = {Dereziński, Jan and Napiórkowski, Marcin M},
  issn         = {1424-0637},
  journal      = {Annales Henri Poincaré},
  number       = {12},
  pages        = {2409--2439},
  publisher    = {Springer Nature},
  title        = {{Excitation spectrum of interacting bosons in the Mean-Field Infinite-Volume limit}},
  doi          = {10.1007/s00023-013-0302-4},
  volume       = {15},
  year         = {2014},
}

@article{2341,
  abstract     = {We study the ground state properties of an atom with nuclear charge Z and N bosonic &quot;electrons&quot; in the presence of a homogeneous magnetic field B. We investigate the mean field limit N→∞ with N / Z fixed, and identify three different asymptotic regions, according to B≪Z2,B∼Z2,andB≫Z2 . In Region 1 standard Hartree theory is applicable. Region 3 is described by a one-dimensional functional, which is identical to the so-called Hyper-Strong functional introduced by Lieb, Solovej and Yngvason for atoms with fermionic electrons in the region B≫Z3 ; i.e., for very strong magnetic fields the ground state properties of atoms are independent of statistics. For Region 2 we introduce a general magnetic Hartree functional, which is studied in detail. It is shown that in the special case of an atom it can be restricted to the subspace of zero angular momentum parallel to the magnetic field, which simplifies the theory considerably. The functional reproduces the energy and the one-particle reduced density matrix for the full N-particle ground state to leading order in N, and it implies the description of the other regions as limiting cases.},
  author       = {Baumgartner, Bernhard and Seiringer, Robert},
  issn         = {1424-0637},
  journal      = {Annales Henri Poincare},
  number       = {1},
  pages        = {41 -- 76},
  publisher    = {Birkhäuser},
  title        = {{Atoms with bosonic &quot;electrons&quot; in strong magnetic fields}},
  doi          = {10.1007/PL00001032},
  volume       = {2},
  year         = {2001},
}

