284 research outputs found
Electronic double-excitations in quantum wells: solving the two-time Kadanoff-Baym equations
For a quantum many-body system, the direct population of states of
double-excitation character is a clear indication that correlations importantly
contribute to its nonequilibrium properties. We analyze such
correlation-induced transitions by propagating the nonequilibrium Green's
functions in real-time within the second Born approximation. As crucial
benchmarks, we compute the absorption spectrum of few electrons confined in
quantum wells of different width. Our results include the full two-time
solution of the Kadanoff-Baym equations as well as of their time-diagonal limit
and are compared to Hartree-Fock and exact diagonalization data
Non-equilibrium Green's function approach to inhomogeneous quantum many-body systems using the Generalized Kadanoff Baym Ansatz
In non-equilibrium Green's function calculations the use of the Generalized
Kadanoff-Baym Ansatz (GKBA) allows for a simple approximate reconstruction of
the two-time Green's function from its time-diagonal value. With this a drastic
reduction of the computational needs is achieved in time-dependent
calculations, making longer time propagation possible and more complex systems
accessible. This paper gives credit to the GKBA that was introduced 25 years
ago. After a detailed derivation of the GKBA, we recall its application to
homogeneous systems and show how to extend it to strongly correlated,
inhomogeneous systems. As a proof of concept, we present results for a
2-electron quantum well, where the correct treatment of the correlated electron
dynamics is crucial for the correct description of the equilibrium and dynamic
properties
Invariance of the Kohn (sloshing) mode in a conserving theory
It is proven that the center of mass (COM or Kohn) oscillation of a many-body
system in a harmonic trap coincides with the motion of a single particle as
long as conserving approximations are applied to treat the interactions. The
two conditions formulated by Kadanoff and Baym \cite{kb-book} are shown to be
sufficient to preserve the COM mode. The result equally applies to zero and
finite temperature, as well as to nonequilibrium situations, and to the linear
and nonlinear response regimes
Electronic correlations in double ionization of atoms in pump-probe experiments
The ionization dynamics of a two-electron atom in an attosecond XUV-infrared
pump-probe experiment is simulated by solving the time-dependent two-electron
Schr\"odinger equation. A dramatic change of the double ionization (DI) yield
with variation of the pump-probe delay is reported and the governing role of
electron-electron correlations is shown. The results allow for a direct control
of the DI yield and of the relative strength of double and single ionization
On the Coulomb-dipole transition in mesoscopic classical and quantum electron-hole bilayers
We study the Coulomb-to-dipole transition which occurs when the separation
of an electron-hole bilayer system is varied with respect to the
characteristic in-layer distances. An analysis of the classical ground state
configurations for harmonically confined clusters with reveals that
the energetically most favorable state can differ from that of two-dimensional
pure dipole or Coulomb systems. Performing a normal mode analysis for the N=19
cluster it is found that the lowest mode frequencies exhibit drastic changes
when is varied. Furthermore, we present quantum-mechanical ground states
for N=6, 10 and 12 spin-polarized electrons and holes. We compute the
single-particle energies and orbitals in self-consistent Hartree-Fock
approximation over a broad range of layer separations and coupling strengths
between the limits of the ideal Fermi gas and the Wigner crystal
Short time dynamics with initial correlations
The short-time dynamics of correlated systems is strongly influenced by
initial correlations giving rise to an additional collision integral in the
non-Markovian kinetic equation. Exact cancellation of the two integrals is
found if the initial state is thermal equilibrium which is an important
consistency criterion. Analytical results are given for the time evolution of
the correlation energy which are confirmed by comparisons with molecular
dynamics simulations (MD)
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