The change in energy of an ideal Fermi gas when a local one-body potential is inserted into the system, or when the density is changed locally, are important quantities in condensed matter physics. We show that they can be rigorously bounded from below by a universal constant times the value given by the semiclassical approximation
Quantum effects of bulk matter, in the form of massive fermions, are considered in the Randall-Sundr...
The Debye mass m_D is computed nonperturbatively in the deconfined phase of QCD, where chromomagneti...
We implement and apply time-dependent density matrix renormalization group (TD-DMRG) algorithms at z...
The change in energy of an ideal Fermi gas when a local one-body potential is inserted into the syst...
The change in energy of an ideal Fermi gas when a local one-body potential is inserted into the syst...
We show that the Born-Oppenheimer potential energy surface in Kohn-Sham theory behaves like the corr...
Using the general form of the static energy solutions to the Dirac equation with a magnetic field, w...
Part fourteen of course materials for Statistical Physics I: PHY525, taught by Gerhard Müller at the...
The most widely-used density functionals for the exchange-correlation energy are inexact for one-ele...
The system we consider here is a charged fermions gas in the effective mass approximation, and in gr...
Cooled down and diluted quark-gluon matter is considered. A possibility of condensation of multiquar...
Author Institution: Institut fur Theoretische Chemie, Universitat zu Koln, Greinstr. 4, D-50939 Koln...
AbstractThe phase diagram of the Gross–Neveu (GN) model in 2+1 dimensions as a function of chemical ...
Part twelve of course materials for Statistical Physics I: PHY525, taught by Gerhard Müller at the U...
The total energy and action, which is stored in the flux-tube between a static quark-antiquark pair,...
Quantum effects of bulk matter, in the form of massive fermions, are considered in the Randall-Sundr...
The Debye mass m_D is computed nonperturbatively in the deconfined phase of QCD, where chromomagneti...
We implement and apply time-dependent density matrix renormalization group (TD-DMRG) algorithms at z...
The change in energy of an ideal Fermi gas when a local one-body potential is inserted into the syst...
The change in energy of an ideal Fermi gas when a local one-body potential is inserted into the syst...
We show that the Born-Oppenheimer potential energy surface in Kohn-Sham theory behaves like the corr...
Using the general form of the static energy solutions to the Dirac equation with a magnetic field, w...
Part fourteen of course materials for Statistical Physics I: PHY525, taught by Gerhard Müller at the...
The most widely-used density functionals for the exchange-correlation energy are inexact for one-ele...
The system we consider here is a charged fermions gas in the effective mass approximation, and in gr...
Cooled down and diluted quark-gluon matter is considered. A possibility of condensation of multiquar...
Author Institution: Institut fur Theoretische Chemie, Universitat zu Koln, Greinstr. 4, D-50939 Koln...
AbstractThe phase diagram of the Gross–Neveu (GN) model in 2+1 dimensions as a function of chemical ...
Part twelve of course materials for Statistical Physics I: PHY525, taught by Gerhard Müller at the U...
The total energy and action, which is stored in the flux-tube between a static quark-antiquark pair,...
Quantum effects of bulk matter, in the form of massive fermions, are considered in the Randall-Sundr...
The Debye mass m_D is computed nonperturbatively in the deconfined phase of QCD, where chromomagneti...
We implement and apply time-dependent density matrix renormalization group (TD-DMRG) algorithms at z...