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 -