TY - JOUR
AB - We give a bound on the ground-state energy of a system of N non-interacting fermions in a three-dimensional cubic box interacting with an impurity particle via point interactions. We show that the change in energy compared to the system in the absence of the impurity is bounded in terms of the gas density and the scattering length of the interaction, independently of N. Our bound holds as long as the ratio of the mass of the impurity to the one of the gas particles is larger than a critical value m∗ ∗≈ 0.36 , which is the same regime for which we recently showed stability of the system.
AU - Moser, Thomas
AU - Seiringer, Robert
ID - 5856
IS - 4
JF - Annales Henri Poincare
SN - 14240637
TI - Energy contribution of a point-interacting impurity in a Fermi gas
VL - 20
ER -
TY - JOUR
AB - 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.
AU - Leopold, Nikolai K
AU - Petrat, Sören P
ID - 6788
IS - 10
JF - Annales Henri Poincare
SN - 1424-0637
TI - Mean-field dynamics for the Nelson model with fermions
VL - 20
ER -
TY - JOUR
AB - We discuss thermodynamic properties of harmonically trapped
imperfect quantum gases. The spatial inhomogeneity of these systems imposes
a redefinition of the mean-field interparticle potential energy as compared
to the homogeneous case. In our approach, it takes the form a
2N2 ωd, where
N is the number of particles, ω—the harmonic trap frequency, d—system’s
dimensionality, and a is a parameter characterizing the interparticle interaction.
We provide arguments that this model corresponds to the limiting case of
a long-ranged interparticle potential of vanishingly small amplitude. This
conclusion is drawn from a computation similar to the well-known Kac scaling
procedure, which is presented here in a form adapted to the case of an isotropic
harmonic trap. We show that within the model, the imperfect gas of trapped
repulsive bosons undergoes the Bose–Einstein condensation provided d > 1.
The main result of our analysis is that in d = 1 the gas of attractive imperfect
fermions with a = −aF < 0 is thermodynamically equivalent to the gas of
repulsive bosons with a = aB > 0 provided the parameters aF and aB fulfill
the relation aB + aF = . This result supplements similar recent conclusion
about thermodynamic equivalence of two-dimensional (2D) uniform imperfect
repulsive Bose and attractive Fermi gases.
AU - Mysliwy, Krzysztof
AU - Napiórkowski, Marek
ID - 6840
IS - 6
JF - Journal of Statistical Mechanics: Theory and Experiment
TI - Thermodynamics of inhomogeneous imperfect quantum gases in harmonic traps
VL - 2019
ER -
TY - JOUR
AB - We consider systems of bosons trapped in a box, in the Gross–Pitaevskii regime. We show that low-energy states exhibit complete Bose–Einstein condensation with an optimal bound on the number of orthogonal excitations. This extends recent results obtained in Boccato et al. (Commun Math Phys 359(3):975–1026, 2018), removing the assumption of small interaction potential.
AU - Boccato, Chiara
AU - Brennecke, Christian
AU - Cenatiempo, Serena
AU - Schlein, Benjamin
ID - 6906
JF - Communications in Mathematical Physics
SN - 0010-3616
TI - Optimal rate for Bose-Einstein condensation in the Gross-Pitaevskii regime
VL - 376
ER -
TY - JOUR
AB - We modify the "floating crystal" trial state for the classical homogeneous electron gas (also known as jellium), in order to suppress the boundary charge fluctuations that are known to lead to a macroscopic increase of the energy. The argument is to melt a thin layer of the crystal close to the boundary and consequently replace it by an incompressible fluid. With the aid of this trial state we show that three different definitions of the ground-state energy of jellium coincide. In the first point of view the electrons are placed in a neutralizing uniform background. In the second definition there is no background but the electrons are submitted to the constraint that their density is constant, as is appropriate in density functional theory. Finally, in the third system each electron interacts with a periodic image of itself; that is, periodic boundary conditions are imposed on the interaction potential.
AU - Lewin, Mathieu
AU - Lieb, Elliott H.
AU - Seiringer, Robert
ID - 7015
IS - 3
JF - Physical Review B
SN - 2469-9950
TI - Floating Wigner crystal with no boundary charge fluctuations
VL - 100
ER -
TY - JOUR
AB - We present microscopic derivations of the defocusing two-dimensional cubic nonlinear Schrödinger equation and the Gross–Pitaevskii equation starting froman interacting N-particle system of bosons. We consider the interaction potential to be given either by Wβ(x)=N−1+2βW(Nβx), for any β>0, or to be given by VN(x)=e2NV(eNx), for some spherical symmetric, nonnegative and compactly supported W,V∈L∞(R2,R). In both cases we prove the convergence of the reduced density corresponding to the exact time evolution to the projector onto the solution of the corresponding nonlinear Schrödinger equation in trace norm. For the latter potential VN we show that it is crucial to take the microscopic structure of the condensate into account in order to obtain the correct dynamics.
AU - Jeblick, Maximilian
AU - Leopold, Nikolai K
AU - Pickl, Peter
ID - 7100
IS - 1
JF - Communications in Mathematical Physics
SN - 0010-3616
TI - Derivation of the time dependent Gross–Pitaevskii equation in two dimensions
VL - 372
ER -
TY - JOUR
AB - We prove upper and lower bounds on the ground-state energy of the ideal two-dimensional anyon gas. Our bounds are extensive in the particle number, as for fermions, and linear in the statistics parameter (Formula presented.). The lower bounds extend to Lieb–Thirring inequalities for all anyons except bosons.
AU - Lundholm, Douglas
AU - Seiringer, Robert
ID - 295
IS - 11
JF - Letters in Mathematical Physics
TI - Fermionic behavior of ideal anyons
VL - 108
ER -
TY - JOUR
AB - In this paper we define and study the classical Uniform Electron Gas (UEG), a system of infinitely many electrons whose density is constant everywhere in space. The UEG is defined differently from Jellium, which has a positive constant background but no constraint on the density. We prove that the UEG arises in Density Functional Theory in the limit of a slowly varying density, minimizing the indirect Coulomb energy. We also construct the quantum UEG and compare it to the classical UEG at low density.
AU - Lewi, Mathieu
AU - Lieb, Élliott
AU - Seiringer, Robert
ID - 180
JF - Journal de l'Ecole Polytechnique - Mathematiques
TI - Statistical mechanics of the uniform electron gas
VL - 5
ER -
TY - THES
AB - In this thesis we will discuss systems of point interacting fermions, their stability and other spectral properties. Whereas for bosons a point interacting system is always unstable this ques- tion is more subtle for a gas of two species of fermions. In particular the answer depends on the mass ratio between these two species. Most of this work will be focused on the N + M model which consists of two species of fermions with N, M particles respectively which interact via point interactions. We will introduce this model using a formal limit and discuss the N + 1 system in more detail. In particular, we will show that for mass ratios above a critical one, which does not depend on the particle number, the N + 1 system is stable. In the context of this model we will prove rigorous versions of Tan relations which relate various quantities of the point-interacting model. By restricting the N + 1 system to a box we define a finite density model with point in- teractions. In the context of this system we will discuss the energy change when introducing a point-interacting impurity into a system of non-interacting fermions. We will see that this change in energy is bounded independently of the particle number and in particular the bound only depends on the density and the scattering length. As another special case of the N + M model we will show stability of the 2 + 2 model for mass ratios in an interval around one. Further we will investigate a different model of point interactions which was discussed before in the literature and which is, contrary to the N + M model, not given by a limiting procedure but is based on a Dirichlet form. We will show that this system behaves trivially in the thermodynamic limit, i.e. the free energy per particle is the same as the one of the non-interacting system.
AU - Moser, Thomas
ID - 52
TI - Point interactions in systems of fermions
ER -
TY - JOUR
AB - We analyse the canonical Bogoliubov free energy functional in three dimensions at low temperatures in the dilute limit. We prove existence of a first-order phase transition and, in the limit (Formula presented.), we determine the critical temperature to be (Formula presented.) to leading order. Here, (Formula presented.) is the critical temperature of the free Bose gas, ρ is the density of the gas and a is the scattering length of the pair-interaction potential V. We also prove asymptotic expansions for the free energy. In particular, we recover the Lee–Huang–Yang formula in the limit (Formula presented.).
AU - Napiórkowski, Marcin M
AU - Reuvers, Robin
AU - Solovej, Jan
ID - 554
IS - 1
JF - Communications in Mathematical Physics
SN - 00103616
TI - The Bogoliubov free energy functional II: The dilute Limit
VL - 360
ER -
TY - JOUR
AB - We study a quantum impurity possessing both translational and internal rotational degrees of freedom interacting with a bosonic bath. Such a system corresponds to a “rotating polaron,” which can be used to model, e.g., a rotating molecule immersed in an ultracold Bose gas or superfluid helium. We derive the Hamiltonian of the rotating polaron and study its spectrum in the weak- and strong-coupling regimes using a combination of variational, diagrammatic, and mean-field approaches. We reveal how the coupling between linear and angular momenta affects stable quasiparticle states, and demonstrate that internal rotation leads to an enhanced self-localization in the translational degrees of freedom.
AU - Yakaboylu, Enderalp
AU - Midya, Bikashkali
AU - Deuchert, Andreas
AU - Leopold, Nikolai K
AU - Lemeshko, Mikhail
ID - 5983
IS - 22
JF - Physical Review B
SN - 2469-9950
TI - Theory of the rotating polaron: Spectrum and self-localization
VL - 98
ER -
TY - JOUR
AB - The Bogoliubov free energy functional is analysed. The functional serves as a model of a translation-invariant Bose gas at positive temperature. We prove the existence of minimizers in the case of repulsive interactions given by a sufficiently regular two-body potential. Furthermore, we prove the existence of a phase transition in this model and provide its phase diagram.
AU - Napiórkowski, Marcin M
AU - Reuvers, Robin
AU - Solovej, Jan Philip
ID - 6002
IS - 3
JF - Archive for Rational Mechanics and Analysis
SN - 0003-9527
TI - The Bogoliubov free energy functional I: Existence of minimizers and phase diagram
VL - 229
ER -
TY - JOUR
AB - We give a lower bound on the ground state energy of a system of two fermions of one species interacting with two fermions of another species via point interactions. We show that there is a critical mass ratio m2 ≈ 0.58 such that the system is stable, i.e., the energy is bounded from below, for m∈[m2,m2−1]. So far it was not known whether this 2 + 2 system exhibits a stable region at all or whether the formation of four-body bound states causes an unbounded spectrum for all mass ratios, similar to the Thomas effect. Our result gives further evidence for the stability of the more general N + M system.
AU - Moser, Thomas
AU - Seiringer, Robert
ID - 154
IS - 3
JF - Mathematical Physics Analysis and Geometry
SN - 13850172
TI - Stability of the 2+2 fermionic system with point interactions
VL - 21
ER -
TY - CONF
AB - We report on a novel strategy to derive mean-field limits of quantum mechanical systems in which a large number of particles weakly couple to a second-quantized radiation field. The technique combines the method of counting and the coherent state approach to study the growth of the correlations among the particles and in the radiation field. As an instructional example, we derive the Schrödinger–Klein–Gordon system of equations from the Nelson model with ultraviolet cutoff and possibly massless scalar field. In particular, we prove the convergence of the reduced density matrices (of the nonrelativistic particles and the field bosons) associated with the exact time evolution to the projectors onto the solutions of the Schrödinger–Klein–Gordon equations in trace norm. Furthermore, we derive explicit bounds on the rate of convergence of the one-particle reduced density matrix of the nonrelativistic particles in Sobolev norm.
AU - Leopold, Nikolai K
AU - Pickl, Peter
ID - 11
TI - Mean-field limits of particles in interaction with quantised radiation fields
VL - 270
ER -
TY - JOUR
AB - Following an earlier calculation in 3D, we calculate the 2D critical temperature of a dilute, translation-invariant Bose gas using a variational formulation of the Bogoliubov approximation introduced by Critchley and Solomon in 1976. This provides the first analytical calculation of the Kosterlitz-Thouless transition temperature that includes the constant in the logarithm.
AU - Napiórkowski, Marcin M
AU - Reuvers, Robin
AU - Solovej, Jan
ID - 399
IS - 1
JF - EPL
TI - Calculation of the critical temperature of a dilute Bose gas in the Bogoliubov approximation
VL - 121
ER -
TY - JOUR
AB - We consider the two-dimensional BCS functional with a radial pair interaction. We show that the translational symmetry is not broken in a certain temperature interval below the critical temperature. In the case of vanishing angular momentum, our results carry over to the three-dimensional case.
AU - Deuchert, Andreas
AU - Geisinge, Alissa
AU - Hainzl, Christian
AU - Loss, Michael
ID - 400
IS - 5
JF - Annales Henri Poincare
TI - Persistence of translational symmetry in the BCS model with radial pair interaction
VL - 19
ER -
TY - JOUR
AB - 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.
AU - Frank, Rupert
AU - Phan Thanh, Nam
AU - Van Den Bosch, Hanne
ID - 446
IS - 3
JF - Communications on Pure and Applied Mathematics
TI - The ionization conjecture in Thomas–Fermi–Dirac–von Weizsäcker theory
VL - 71
ER -
TY - JOUR
AB - The derivation of effective evolution equations is central to the study of non-stationary quantum many-body systems, and widely used in contexts such as superconductivity, nuclear physics, Bose–Einstein condensation and quantum chemistry. We reformulate the Dirac–Frenkel approximation principle in terms of reduced density matrices and apply it to fermionic and bosonic many-body systems. We obtain the Bogoliubov–de Gennes and Hartree–Fock–Bogoliubov equations, respectively. While we do not prove quantitative error estimates, our formulation does show that the approximation is optimal within the class of quasifree states. Furthermore, we prove well-posedness of the Bogoliubov–de Gennes equations in energy space and discuss conserved quantities
AU - Benedikter, Niels P
AU - Sok, Jérémy
AU - Solovej, Jan
ID - 455
IS - 4
JF - Annales Henri Poincare
TI - The Dirac–Frenkel principle for reduced density matrices and the Bogoliubov–de Gennes equations
VL - 19
ER -
TY - JOUR
AB - 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.
AU - Nam, Phan
AU - Napiórkowski, Marcin M
ID - 739
IS - 5
JF - Journal de Mathématiques Pures et Appliquées
SN - 00217824
TI - A note on the validity of Bogoliubov correction to mean field dynamics
VL - 108
ER -
TY - JOUR
AB - We prove that a system of N fermions interacting with an additional particle via point interactions is stable if the ratio of the mass of the additional particle to the one of the fermions is larger than some critical m*. The value of m* is independent of N and turns out to be less than 1. This fact has important implications for the stability of the unitary Fermi gas. We also characterize the domain of the Hamiltonian of this model, and establish the validity of the Tan relations for all wave functions in the domain.
AU - Moser, Thomas
AU - Seiringer, Robert
ID - 741
IS - 1
JF - Communications in Mathematical Physics
SN - 00103616
TI - Stability of a fermionic N+1 particle system with point interactions
VL - 356
ER -
TY - JOUR
AB - 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.
AU - Nam, Phan
AU - Napiórkowski, Marcin M
ID - 484
IS - 3
JF - Advances in Theoretical and Mathematical Physics
SN - 10950761
TI - Bogoliubov correction to the mean-field dynamics of interacting bosons
VL - 21
ER -
TY - JOUR
AB - 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.
AU - Lewin, Mathieu
AU - Nam, Phan
AU - Rougerie, Nicolas
ID - 632
IS - 6
JF - Proceedings of the American Mathematical Society
TI - A note on 2D focusing many boson systems
VL - 145
ER -
TY - JOUR
AB - 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.
AU - Nam, Phan
AU - Van Den Bosch, Hanne
ID - 1079
IS - 2
JF - Mathematical Physics, Analysis and Geometry
SN - 13850172
TI - Nonexistence in Thomas Fermi-Dirac-von Weizsäcker theory with small nuclear charges
VL - 20
ER -
TY - JOUR
AB - The existence of a self-localization transition in the polaron problem has been under an active debate ever since Landau suggested it 83 years ago. Here we reveal the self-localization transition for the rotational analogue of the polaron -- the angulon quasiparticle. We show that, unlike for the polarons, self-localization of angulons occurs at finite impurity-bath coupling already at the mean-field level. The transition is accompanied by the spherical-symmetry breaking of the angulon ground state and a discontinuity in the first derivative of the ground-state energy. Moreover, the type of the symmetry breaking is dictated by the symmetry of the microscopic impurity-bath interaction, which leads to a number of distinct self-localized states. The predicted effects can potentially be addressed in experiments on cold molecules trapped in superfluid helium droplets and ultracold quantum gases, as well as on electronic excitations in solids and Bose-Einstein condensates.
AU - Li, Xiang
AU - Seiringer, Robert
AU - Lemeshko, Mikhail
ID - 1120
IS - 3
JF - Physical Review A
SN - 24699926
TI - Angular self-localization of impurities rotating in a bosonic bath
VL - 95
ER -
TY - JOUR
AB - We consider a model of fermions interacting via point interactions, defined via a certain weighted Dirichlet form. While for two particles the interaction corresponds to infinite scattering length, the presence of further particles effectively decreases the interaction strength. We show that the model becomes trivial in the thermodynamic limit, in the sense that the free energy density at any given particle density and temperature agrees with the corresponding expression for non-interacting particles.
AU - Moser, Thomas
AU - Seiringer, Robert
ID - 1198
IS - 3
JF - Letters in Mathematical Physics
SN - 03779017
TI - Triviality of a model of particles with point interactions in the thermodynamic limit
VL - 107
ER -
TY - JOUR
AB - We consider a many-body system of fermionic atoms interacting via a local pair potential and subject to an external potential within the framework of Bardeen-Cooper-Schrieffer (BCS) theory. We measure the free energy of the whole sample with respect to the free energy of a reference state which allows us to define a BCS functional with boundary conditions at infinity. Our main result is a lower bound for this energy functional in terms of expressions that typically appear in Ginzburg-Landau functionals.
AU - Deuchert, Andreas
ID - 912
IS - 8
JF - Journal of Mathematical Physics
SN - 00222488
TI - A lower bound for the BCS functional with boundary conditions at infinity
VL - 58
ER -
TY - JOUR
AB - Recently it was shown that molecules rotating in superfluid helium can be described in terms of the angulon quasiparticles (Phys. Rev. Lett. 118, 095301 (2017)). Here we demonstrate that in the experimentally realized regime the angulon can be seen as a point charge on a 2-sphere interacting with a gauge field of a non-abelian magnetic monopole. Unlike in several other settings, the gauge fields of the angulon problem emerge in the real coordinate space, as opposed to the momentum space or some effective parameter space. Furthermore, we find a topological transition associated with making the monopole abelian, which takes place in the vicinity of the previously reported angulon instabilities. These results pave the way for studying topological phenomena in experiments on molecules trapped in superfluid helium nanodroplets, as well as on other realizations of orbital impurity problems.
AU - Yakaboylu, Enderalp
AU - Deuchert, Andreas
AU - Lemeshko, Mikhail
ID - 997
IS - 23
JF - APS Physics, Physical Review Letters
SN - 00319007
TI - Emergence of non-abelian magnetic monopoles in a quantum impurity problem
VL - 119
ER -
TY - JOUR
AB - We consider Ising models in two and three dimensions, with short range ferromagnetic and long range, power-law decaying, antiferromagnetic interactions. We let J be the ratio between the strength of the ferromagnetic to antiferromagnetic interactions. The competition between these two kinds of interactions induces the system to form domains of minus spins in a background of plus spins, or vice versa. If the decay exponent p of the long range interaction is larger than dÂ +Â 1, with d the space dimension, this happens for all values of J smaller than a critical value Jc(p), beyond which the ground state is homogeneous. In this paper, we give a characterization of the infinite volume ground states of the system, for pÂ >Â 2d and J in a left neighborhood of Jc(p). In particular, we prove that the quasi-one-dimensional states consisting of infinite stripes (dÂ =Â 2) or slabs (dÂ =Â 3), all of the same optimal width and orientation, and alternating magnetization, are infinite volume ground states. Our proof is based on localization bounds combined with reflection positivity.
AU - Giuliani, Alessandro
AU - Seiringer, Robert
ID - 1291
IS - 3
JF - Communications in Mathematical Physics
TI - Periodic striped ground states in Ising models with competing interactions
VL - 347
ER -
TY - JOUR
AB - We study the time-dependent Bogoliubov–de-Gennes equations for generic translation-invariant fermionic many-body systems. For initial states that are close to thermal equilibrium states at temperatures near the critical temperature, we show that the magnitude of the order parameter stays approximately constant in time and, in particular, does not follow a time-dependent Ginzburg–Landau equation, which is often employed as a phenomenological description and predicts a decay of the order parameter in time. The full non-linear structure of the equations is necessary to understand this behavior.
AU - Frank, Rupert
AU - Hainzl, Christian
AU - Schlein, Benjamin
AU - Seiringer, Robert
ID - 1422
IS - 7
JF - Letters in Mathematical Physics
TI - Incompatibility of time-dependent Bogoliubov–de-Gennes and Ginzburg–Landau equations
VL - 106
ER -
TY - CONF
AB - We report on a mathematically rigorous analysis of the superfluid properties of a Bose- Einstein condensate in the many-body ground state of a one-dimensional model of interacting bosons in a random potential.
AU - Könenberg, Martin
AU - Moser, Thomas
AU - Seiringer, Robert
AU - Yngvason, Jakob
ID - 1428
IS - 1
T2 - Journal of Physics: Conference Series
TI - Superfluidity and BEC in a Model of Interacting Bosons in a Random Potential
VL - 691
ER -
TY - JOUR
AB - We study the time evolution of a system of N spinless fermions in R3 which interact through a pair potential, e.g., the Coulomb potential. We compare the dynamics given by the solution to Schrödinger's equation with the time-dependent Hartree-Fock approximation, and we give an estimate for the accuracy of this approximation in terms of the kinetic energy of the system. This leads, in turn, to bounds in terms of the initial total energy of the system.
AU - Bach, Volker
AU - Breteaux, Sébastien
AU - Petrat, Sören P
AU - Pickl, Peter
AU - Tzaneteas, Tim
ID - 1436
IS - 1
JF - Journal de Mathématiques Pures et Appliquées
TI - Kinetic energy estimates for the accuracy of the time-dependent Hartree-Fock approximation with Coulomb interaction
VL - 105
ER -
TY - JOUR
AB - We consider the Tonks-Girardeau gas subject to a random external potential. If the disorder is such that the underlying one-particle Hamiltonian displays localization (which is known to be generically the case), we show that there is exponential decay of correlations in the many-body eigenstates. Moreover, there is no Bose-Einstein condensation and no superfluidity, even at zero temperature.
AU - Seiringer, Robert
AU - Warzel, Simone
ID - 1478
IS - 3
JF - New Journal of Physics
TI - Decay of correlations and absence of superfluidity in the disordered Tonks-Girardeau gas
VL - 18
ER -
TY - JOUR
AB - We review recent results concerning the mathematical properties of the Bardeen-Cooper-Schrieffer (BCS) functional of superconductivity, which were obtained in a series of papers, partly in collaboration with R. Frank, E. Hamza, S. Naboko, and J. P. Solovej. Our discussion includes, in particular, an investigation of the critical temperature for a general class of interaction potentials, as well as a study of its dependence on external fields. We shall explain how the Ginzburg-Landau model can be derived from the BCS theory in a suitable parameter regime.
AU - Hainzl, Christian
AU - Seiringer, Robert
ID - 1486
IS - 2
JF - Journal of Mathematical Physics
TI - The Bardeen–Cooper–Schrieffer functional of superconductivity and its mathematical properties
VL - 57
ER -
TY - JOUR
AB - 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.
AU - Lewin, Mathieu
AU - Nam, Phan
AU - Rougerie, Nicolas
ID - 1491
IS - 9
JF - Transactions of the American Mathematical Society
TI - The mean-field approximation and the non-linear Schrödinger functional for trapped Bose gases
VL - 368
ER -
TY - JOUR
AB - We introduce a new method for deriving the time-dependent Hartree or Hartree-Fock equations as an effective mean-field dynamics from the microscopic Schrödinger equation for fermionic many-particle systems in quantum mechanics. The method is an adaption of the method used in Pickl (Lett. Math. Phys. 97 (2) 151–164 2011) for bosonic systems to fermionic systems. It is based on a Gronwall type estimate for a suitable measure of distance between the microscopic solution and an antisymmetrized product state. We use this method to treat a new mean-field limit for fermions with long-range interactions in a large volume. Some of our results hold for singular attractive or repulsive interactions. We can also treat Coulomb interaction assuming either a mild singularity cutoff or certain regularity conditions on the solutions to the Hartree(-Fock) equations. In the considered limit, the kinetic and interaction energy are of the same order, while the average force is subleading. For some interactions, we prove that the Hartree(-Fock) dynamics is a more accurate approximation than a simpler dynamics that one would expect from the subleading force. With our method we also treat the mean-field limit coupled to a semiclassical limit, which was discussed in the literature before, and we recover some of the previous results. All results hold for initial data close (but not necessarily equal) to antisymmetrized product states and we always provide explicit rates of convergence.
AU - Petrat, Sören P
AU - Pickl, Peter
ID - 1493
IS - 1
JF - Mathematical Physics, Analysis and Geometry
TI - A new method and a new scaling for deriving fermionic mean-field dynamics
VL - 19
ER -
TY - JOUR
AB - 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.
AU - Nam, Phan
AU - Napiórkowski, Marcin M
AU - Solovej, Jan
ID - 1545
IS - 11
JF - Journal of Functional Analysis
TI - Diagonalization of bosonic quadratic Hamiltonians by Bogoliubov transformations
VL - 270
ER -
TY - JOUR
AB - 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.
AU - Frank, Rupert
AU - Hainzl, Christian
AU - Seiringer, Robert
AU - Solovej, Jan
ID - 1620
IS - 1
JF - Communications in Mathematical Physics
TI - The external field dependence of the BCS critical temperature
VL - 342
ER -
TY - JOUR
AB - 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.
AU - Lundholm, Douglas
AU - Nam, Phan
AU - Portmann, Fabian
ID - 1622
IS - 3
JF - Archive for Rational Mechanics and Analysis
TI - Fractional Hardy–Lieb–Thirring and related Inequalities for interacting systems
VL - 219
ER -
TY - JOUR
AB - 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.
AU - Nam, Phan
AU - Rougerie, Nicolas
AU - Seiringer, Robert
ID - 1143
IS - 2
JF - Analysis and PDE
TI - Ground states of large bosonic systems: The gross Pitaevskii limit revisited
VL - 9
ER -
TY - JOUR
AB - We consider the Bogolubov–Hartree–Fock functional for a fermionic many-body system with two-body interactions. For suitable interaction potentials that have a strong enough attractive tail in order to allow for two-body bound states, but are otherwise sufficiently repulsive to guarantee stability of the system, we show that in the low-density limit the ground state of this model consists of a Bose–Einstein condensate of fermion pairs. The latter can be described by means of the Gross–Pitaevskii energy functional.
AU - Bräunlich, Gerhard
AU - Hainzl, Christian
AU - Seiringer, Robert
ID - 1259
IS - 2
JF - Mathematical Physics, Analysis and Geometry
TI - Bogolubov–Hartree–Fock theory for strongly interacting fermions in the low density limit
VL - 19
ER -
TY - JOUR
AB - 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.
AU - Frank, Rupert
AU - Killip, Rowan
AU - Nam, Phan
ID - 1267
IS - 8
JF - Letters in Mathematical Physics
TI - Nonexistence of large nuclei in the liquid drop model
VL - 106
ER -
TY - JOUR
AB - Given a convex function (Formula presented.) and two hermitian matrices A and B, Lewin and Sabin study in (Lett Math Phys 104:691–705, 2014) the relative entropy defined by (Formula presented.). Among other things, they prove that the so-defined quantity is monotone if and only if (Formula presented.) is operator monotone. The monotonicity is then used to properly define (Formula presented.) for bounded self-adjoint operators acting on an infinite-dimensional Hilbert space by a limiting procedure. More precisely, for an increasing sequence of finite-dimensional projections (Formula presented.) with (Formula presented.) strongly, the limit (Formula presented.) is shown to exist and to be independent of the sequence of projections (Formula presented.). The question whether this sequence converges to its "obvious" limit, namely (Formula presented.), has been left open. We answer this question in principle affirmatively and show that (Formula presented.). If the operators A and B are regular enough, that is (A − B), (Formula presented.) and (Formula presented.) are trace-class, the identity (Formula presented.) holds.
AU - Deuchert, Andreas
AU - Hainzl, Christian
AU - Seiringer, Robert
ID - 1704
IS - 10
JF - Letters in Mathematical Physics
TI - Note on a family of monotone quantum relative entropies
VL - 105
ER -
TY - JOUR
AB - We study a double Cahn-Hilliard type functional related to the Gross-Pitaevskii energy of two-components Bose-Einstein condensates. In the case of large but same order intercomponent and intracomponent coupling strengths, we prove Γ-convergence to a perimeter minimisation functional with an inhomogeneous surface tension. We study the asymptotic behavior of the surface tension as the ratio between the intercomponent and intracomponent coupling strengths becomes very small or very large and obtain good agreement with the physical literature. We obtain as a consequence, symmetry breaking of the minimisers for the harmonic potential.
AU - Goldman, Michael
AU - Royo-Letelier, Jimena
ID - 1807
IS - 3
JF - ESAIM - Control, Optimisation and Calculus of Variations
TI - Sharp interface limit for two components Bose-Einstein condensates
VL - 21
ER -
TY - JOUR
AB - We investigate the relation between Bose-Einstein condensation (BEC) and superfluidity in the ground state of a one-dimensional model of interacting bosons in a strong random potential. We prove rigorously that in a certain parameter regime the superfluid fraction can be arbitrarily small while complete BEC prevails. In another regime there is both complete BEC and complete superfluidity, despite the strong disorder
AU - Könenberg, Martin
AU - Moser, Thomas
AU - Seiringer, Robert
AU - Yngvason, Jakob
ID - 1880
JF - New Journal of Physics
TI - Superfluid behavior of a Bose-Einstein condensate in a random potential
VL - 17
ER -
TY - JOUR
AU - Dereziński, Jan
AU - Napiórkowski, Marcin M
ID - 1939
IS - 7
JF - Annales Henri Poincare
TI - Erratum to: Excitation spectrum of interacting bosons in the Mean-Field Infinite-Volume limit
VL - 16
ER -
TY - JOUR
AB - 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.
AU - Nam, Phan
AU - Seiringer, Robert
ID - 2085
IS - 2
JF - Archive for Rational Mechanics and Analysis
TI - Collective excitations of Bose gases in the mean-field regime
VL - 215
ER -
TY - JOUR
AB - 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.
AU - Lewin, Mathieu
AU - Phan Thanh, Nam
AU - Rougerie, Nicolas
ID - 473
JF - Journal de l'Ecole Polytechnique - Mathematiques
TI - Derivation of nonlinear gibbs measures from many-body quantum mechanics
VL - 2
ER -
TY - JOUR
AB - We consider the quantum ferromagnetic Heisenberg model in three dimensions, for all spins S ≥ 1/2. We rigorously prove the validity of the spin-wave approximation for the excitation spectrum, at the level of the first non-trivial contribution to the free energy at low temperatures. Our proof comes with explicit, constructive upper and lower bounds on the error term. It uses in an essential way the bosonic formulation of the model in terms of the Holstein-Primakoff representation. In this language, the model describes interacting bosons with a hard-core on-site repulsion and a nearest-neighbor attraction. This attractive interaction makes the lower bound on the free energy particularly tricky: the key idea there is to prove a differential inequality for the two-particle density, which is thereby shown to be smaller than the probability density of a suitably weighted two-particle random process on the lattice.
AU - Correggi, Michele
AU - Giuliani, Alessandro
AU - Seiringer, Robert
ID - 1572
IS - 1
JF - Communications in Mathematical Physics
TI - Validity of the spin-wave approximation for the free energy of the Heisenberg ferromagnet
VL - 339
ER -
TY - JOUR
AB - We present a new, simpler proof of the unconditional uniqueness of solutions to the cubic Gross-Pitaevskii hierarchy in ℝ3. One of the main tools in our analysis is the quantum de Finetti theorem. Our uniqueness result is equivalent to the one established in the celebrated works of Erdos, Schlein, and Yau.
AU - Chen, Thomas
AU - Hainzl, Christian
AU - Pavlović, Nataša
AU - Seiringer, Robert
ID - 1573
IS - 10
JF - Communications on Pure and Applied Mathematics
TI - Unconditional uniqueness for the cubic gross pitaevskii hierarchy via quantum de finetti
VL - 68
ER -
TY - CONF
AB - Many questions concerning models in quantum mechanics require a detailed analysis of the spectrum of the corresponding Hamiltonian, a linear operator on a suitable Hilbert space. Of particular relevance for an understanding of the low-temperature properties of a system is the structure of the excitation spectrum, which is the part of the spectrum close to the spectral bottom. We present recent progress on this question for bosonic many-body quantum systems with weak two-body interactions. Such system are currently of great interest, due to their experimental realization in ultra-cold atomic gases. We investigate the accuracy of the Bogoliubov approximations, which predicts that the low-energy spectrum is made up of sums of elementary excitations, with linear dispersion law at low momentum. The latter property is crucial for the superfluid behavior the system.
AU - Seiringer, Robert
ID - 8044
SN - 9788961058063
T2 - Proceeding of the International Congress of Mathematicans
TI - Structure of the excitation spectrum for many-body quantum systems
VL - 3
ER -