@article{446, abstract = {We prove that in Thomas–Fermi–Dirac–von Weizsäcker theory, a nucleus of charge Z > 0 can bind at most Z + C electrons, where C is a universal constant. This result is obtained through a comparison with Thomas-Fermi theory which, as a by-product, gives bounds on the screened nuclear potential and the radius of the minimizer. A key ingredient of the proof is a novel technique to control the particles in the exterior region, which also applies to the liquid drop model with a nuclear background potential.}, author = {Frank, Rupert and Phan Thanh, Nam and Van Den Bosch, Hanne}, journal = {Communications on Pure and Applied Mathematics}, number = {3}, pages = {577 -- 614}, publisher = {Wiley-Blackwell}, title = {{The ionization conjecture in Thomas–Fermi–Dirac–von Weizsäcker theory}}, doi = {10.1002/cpa.21717}, volume = {71}, year = {2018}, } @article{1079, abstract = {We study the ionization problem in the Thomas-Fermi-Dirac-von Weizsäcker theory for atoms and molecules. We prove the nonexistence of minimizers for the energy functional when the number of electrons is large and the total nuclear charge is small. This nonexistence result also applies to external potentials decaying faster than the Coulomb potential. In the case of arbitrary nuclear charges, we obtain the nonexistence of stable minimizers and radial minimizers.}, author = {Nam, Phan and Van Den Bosch, Hanne}, issn = {13850172}, journal = {Mathematical Physics, Analysis and Geometry}, number = {2}, publisher = {Springer}, title = {{Nonexistence in Thomas Fermi-Dirac-von Weizsäcker theory with small nuclear charges}}, doi = {10.1007/s11040-017-9238-0}, volume = {20}, year = {2017}, } @article{739, abstract = {We study the norm approximation to the Schrödinger dynamics of N bosons in with an interaction potential of the form . Assuming that in the initial state the particles outside of the condensate form a quasi-free state with finite kinetic energy, we show that in the large N limit, the fluctuations around the condensate can be effectively described using Bogoliubov approximation for all . The range of β is expected to be optimal for this large class of initial states.}, author = {Nam, Phan and Napiórkowski, Marcin M}, issn = {00217824}, journal = {Journal de Mathématiques Pures et Appliquées}, number = {5}, pages = {662 -- 688}, publisher = {Elsevier}, title = {{A note on the validity of Bogoliubov correction to mean field dynamics}}, doi = {10.1016/j.matpur.2017.05.013}, volume = {108}, year = {2017}, } @article{484, abstract = {We consider the dynamics of a large quantum system of N identical bosons in 3D interacting via a two-body potential of the form N3β-1w(Nβ(x - y)). For fixed 0 = β < 1/3 and large N, we obtain a norm approximation to the many-body evolution in the Nparticle Hilbert space. The leading order behaviour of the dynamics is determined by Hartree theory while the second order is given by Bogoliubov theory.}, author = {Nam, Phan and Napiórkowski, Marcin M}, issn = {10950761}, journal = {Advances in Theoretical and Mathematical Physics}, number = {3}, pages = {683 -- 738}, publisher = {International Press}, title = {{Bogoliubov correction to the mean-field dynamics of interacting bosons}}, doi = {10.4310/ATMP.2017.v21.n3.a4}, volume = {21}, year = {2017}, } @article{632, abstract = {We consider a 2D quantum system of N bosons in a trapping potential |x|s, interacting via a pair potential of the form N2β−1 w(Nβ x). We show that for all 0 < β < (s + 1)/(s + 2), the leading order behavior of ground states of the many-body system is described in the large N limit by the corresponding cubic nonlinear Schrödinger energy functional. Our result covers the focusing case (w < 0) where even the stability of the many-body system is not obvious. This answers an open question mentioned by X. Chen and J. Holmer for harmonic traps (s = 2). Together with the BBGKY hierarchy approach used by these authors, our result implies the convergence of the many-body quantum dynamics to the focusing NLS equation with harmonic trap for all 0 < β < 3/4. }, author = {Lewin, Mathieu and Nam, Phan and Rougerie, Nicolas}, journal = {Proceedings of the American Mathematical Society}, number = {6}, pages = {2441 -- 2454}, publisher = {American Mathematical Society}, title = {{A note on 2D focusing many boson systems}}, doi = {10.1090/proc/13468}, volume = {145}, year = {2017}, } @article{1143, abstract = {We study the ground state of a dilute Bose gas in a scaling limit where the Gross-Pitaevskii functional emerges. This is a repulsive nonlinear Schrödinger functional whose quartic term is proportional to the scattering length of the interparticle interaction potential. We propose a new derivation of this limit problem, with a method that bypasses some of the technical difficulties that previous derivations had to face. The new method is based on a combination of Dyson\'s lemma, the quantum de Finetti theorem and a second moment estimate for ground states of the effective Dyson Hamiltonian. It applies equally well to the case where magnetic fields or rotation are present.}, author = {Nam, Phan and Rougerie, Nicolas and Seiringer, Robert}, journal = {Analysis and PDE}, number = {2}, pages = {459 -- 485}, publisher = {Mathematical Sciences Publishers}, title = {{Ground states of large bosonic systems: The gross Pitaevskii limit revisited}}, doi = {10.2140/apde.2016.9.459}, volume = {9}, year = {2016}, } @article{1622, abstract = {We prove analogues of the Lieb–Thirring and Hardy–Lieb–Thirring inequalities for many-body quantum systems with fractional kinetic operators and homogeneous interaction potentials, where no anti-symmetry on the wave functions is assumed. These many-body inequalities imply interesting one-body interpolation inequalities, and we show that the corresponding one- and many-body inequalities are actually equivalent in certain cases.}, author = {Lundholm, Douglas and Nam, Phan and Portmann, Fabian}, journal = {Archive for Rational Mechanics and Analysis}, number = {3}, pages = {1343 -- 1382}, publisher = {Springer}, title = {{Fractional Hardy–Lieb–Thirring and related Inequalities for interacting systems}}, doi = {10.1007/s00205-015-0923-5}, volume = {219}, year = {2016}, } @article{1491, abstract = {We study the ground state of a trapped Bose gas, starting from the full many-body Schrödinger Hamiltonian, and derive the non-linear Schrödinger energy functional in the limit of a large particle number, when the interaction potential converges slowly to a Dirac delta function. Our method is based on quantitative estimates on the discrepancy between the full many-body energy and its mean-field approximation using Hartree states. These are proved using finite dimensional localization and a quantitative version of the quantum de Finetti theorem. Our approach covers the case of attractive interactions in the regime of stability. In particular, our main new result is a derivation of the 2D attractive non-linear Schrödinger ground state.}, author = {Lewin, Mathieu and Nam, Phan and Rougerie, Nicolas}, journal = {Transactions of the American Mathematical Society}, number = {9}, pages = {6131 -- 6157}, publisher = {American Mathematical Society}, title = {{The mean-field approximation and the non-linear Schrödinger functional for trapped Bose gases}}, doi = {10.1090/tran/6537}, volume = {368}, year = {2016}, } @article{1545, abstract = {We provide general conditions for which bosonic quadratic Hamiltonians on Fock spaces can be diagonalized by Bogoliubov transformations. Our results cover the case when quantum systems have infinite degrees of freedom and the associated one-body kinetic and paring operators are unbounded. Our sufficient conditions are optimal in the sense that they become necessary when the relevant one-body operators commute.}, author = {Nam, Phan and Napiórkowski, Marcin M and Solovej, Jan}, journal = {Journal of Functional Analysis}, number = {11}, pages = {4340 -- 4368}, publisher = {Academic Press}, title = {{Diagonalization of bosonic quadratic Hamiltonians by Bogoliubov transformations}}, doi = {10.1016/j.jfa.2015.12.007}, volume = {270}, year = {2016}, } @article{1267, abstract = {We give a simplified proof of the nonexistence of large nuclei in the liquid drop model and provide an explicit bound. Our bound is within a factor of 2.3 of the conjectured value and seems to be the first quantitative result.}, author = {Frank, Rupert and Killip, Rowan and Nam, Phan}, journal = {Letters in Mathematical Physics}, number = {8}, pages = {1033 -- 1036}, publisher = {Springer}, title = {{Nonexistence of large nuclei in the liquid drop model}}, doi = {10.1007/s11005-016-0860-8}, volume = {106}, year = {2016}, } @article{2085, abstract = {We study the spectrum of a large system of N identical bosons interacting via a two-body potential with strength 1/N. In this mean-field regime, Bogoliubov's theory predicts that the spectrum of the N-particle Hamiltonian can be approximated by that of an effective quadratic Hamiltonian acting on Fock space, which describes the fluctuations around a condensed state. Recently, Bogoliubov's theory has been justified rigorously in the case that the low-energy eigenvectors of the N-particle Hamiltonian display complete condensation in the unique minimizer of the corresponding Hartree functional. In this paper, we shall justify Bogoliubov's theory for the high-energy part of the spectrum of the N-particle Hamiltonian corresponding to (non-linear) excited states of the Hartree functional. Moreover, we shall extend the existing results on the excitation spectrum to the case of non-uniqueness and/or degeneracy of the Hartree minimizer. In particular, the latter covers the case of rotating Bose gases, when the rotation speed is large enough to break the symmetry and to produce multiple quantized vortices in the Hartree minimizer. }, author = {Nam, Phan and Seiringer, Robert}, journal = {Archive for Rational Mechanics and Analysis}, number = {2}, pages = {381 -- 417}, publisher = {Springer}, title = {{Collective excitations of Bose gases in the mean-field regime}}, doi = {10.1007/s00205-014-0781-6}, volume = {215}, year = {2015}, } @article{473, abstract = {We prove that nonlinear Gibbs measures can be obtained from the corresponding many-body, grand-canonical, quantum Gibbs states, in a mean-field limit where the temperature T diverges and the interaction strength behaves as 1/T. We proceed by characterizing the interacting Gibbs state as minimizing a functional counting the free-energy relatively to the non-interacting case. We then perform an infinite-dimensional analogue of phase-space semiclassical analysis, using fine properties of the quantum relative entropy, the link between quantum de Finetti measures and upper/lower symbols in a coherent state basis, as well as Berezin-Lieb type inequalities. Our results cover the measure built on the defocusing nonlinear Schrödinger functional on a finite interval, as well as smoother interactions in dimensions d 2.}, author = {Lewin, Mathieu and Phan Thanh, Nam and Rougerie, Nicolas}, journal = {Journal de l'Ecole Polytechnique - Mathematiques}, pages = {65 -- 115}, publisher = {Ecole Polytechnique}, title = {{Derivation of nonlinear gibbs measures from many-body quantum mechanics}}, doi = {10.5802/jep.18}, volume = {2}, year = {2015}, }