16 research outputs found
Single-particle spectral function for the classical one-component plasma
The spectral function for an electron one-component plasma is calculated
self-consistently using the GW0 approximation for the single-particle
self-energy. In this way, correlation effects which go beyond the mean-field
description of the plasma are contained, i.e. the collisional damping of
single-particle states, the dynamical screening of the interaction and the
appearance of collective plasma modes. Secondly, a novel non-perturbative
analytic solution for the on-shell GW0 self-energy as a function of momentum is
presented. It reproduces the numerical data for the spectral function with a
relative error of less than 10% in the regime where the Debye screening
parameter is smaller than the inverse Bohr radius, kappa<1/a_B. In the limit of
low density, the non-perturbative self-energy behaves as n^(1/4), whereas a
perturbation expansion leads to the unphysical result of a density independent
self-energy [W. Fennel and H. P. Wilfer, Ann. Phys. Lpz._32_, 265 (1974)]. The
derived expression will greatly facilitate the calculation of observables in
correlated plasmas (transport properties, equation of state) that need the
spectral function as an input quantity. This is demonstrated for the shift of
the chemical potential, which is computed from the analytical formulae and
compared to the GW0-result. At a plasma temperature of 100 eV and densities
below 10^21 cm^-3, both approaches deviate less than 10% from each other.Comment: 14 pages, 9 figures accepted for publication in Phys. Rev. E v2:
added section V (application of presented formalism to chemical potential of
the OCP
Partially ionized plasmas in electromagnetic fields
The interaction of partially ionized plasmas with an electromagnetic field is
investigated using quantum statistical methods. A general statistical
expression for the current density of a plasma in an electromagnetic field is
presented and considered in the high field regime. Expressions for the
collisional absorption are derived and discussed. Further, partially ionized
plasmas are considered. Plasma Bloch equations for the description of
bound-free transitions are given and the absorption coefficient as well as rate
coefficients for multiphoton ionization are derived and numerical results are
presented.Comment: 18 pages, 8 figures, accepted for publication in J. Phys.: Conf. Se
Optical properties and one-particle spectral function in non-ideal plasmas
A basic concept to calculate physical features of non-ideal plasmas, such as
optical properties, is the spectral function which is linked to the
self-energy. We calculate the spectral function for a non-relativistic hydrogen
plasma in -approximation. In order to go beyond approximation, we
include self-energy and vertex correction to the polarization function in
lowest order. Partial compensation is observed. The relation of our approach to
and calculations in other fields, such as the band-structure
calculations in semiconductor physics, is discussed. From the spectral function
we derive the absorption coefficient due to inverse bremsstrahlung via the
polarization function. As a result, a significant reduction of the absorption
as compared to the Bethe-Heitler formula for bremsstrahlung is obtained.Comment: 13 pages, 7 figures, 52 references. Submitted to Contrib. Plasma
Phys. Results presented at the International Workshop on Physics of Non-ideal
Plasmas (PNP12), Darmstadt, sept. 4.-8. 200
Ein Fußballer-Roman als Prüfungsgegenstand
1 Hinführung und Zielstellung, 2 Angestrebte Ergebnisse der Entwicklung lexikalischer Kompetenz - vernetzt mit der Entwicklung von Lese-/Textverstehenskompetenz, 3 Arbeit am Wortschatz und Textverstehen - Textanalyse als das Erschließen eines Feldes von Möglichkeiten, 4 Die Tätigkeit des Schülers optimal in Gang setzen - handlungs-regulierende Aufgaben stellen, 5 Literatu
T-matrix approach for the optical spectra of semiconductor heterostructures
Summary form only given. Coulomb correlations are crucial for the realistic computation of semiconductor optical spectra. In low-dimensional systems, band structure and quantum confinement effects play also a major role and have to be integrated in the theory. In our approach, the excited semiconductor is described by nonequilibrium Green's functions for the interacting quasi-particles: carriers, photons, and plasmons, whose time evolution is governed by Dyson equations. Coupled band structure and quantum confinement effects are included in the carrier propagators, and in the transition matrix elements, which give rise to optical selection rules. We show absorption spectra of a 50-A GaAs-AlGaAs QW, as well as corresponding luminescence spectra
Physics and Simulation of Optoelectronic Devices
p. 105-116In low-dimensional systems, quantum-confinement and bandstructure effects strongly influence the many-particle
effects that ultimately give rise to the nonlinear optical properties of semiconductores. In this paper, we use a Keldysh
Greens functions approach to obtain numerical results for isolated quantum wells and coupled superlattices, and
investigate in different limits the combination of band-structure and many-particle effects. The inclusion of higher
order Coulomb correlations gives rise to deviations from the results found in the literature for low carrier densities and
temperatures, which increase with the fundamental band gap, and may be relevant for future optical device design
and operation. The optical spectra presented illustrate the theoretical approach and provide insight on the physical
mechanisms responsible for lasing in wide-band gap heterostructures, as contrasted to the usual 111-V systems