Dispersion Properties of Co-Existing Low Frequency Modes in Quantum Plasmas (original) (raw)

Relativistic quantum plasma dispersion functions

Journal of Physics A: Mathematical and General, 2006

Relativistic quantum plasma dispersion functions are defined and the longitudinal and transverse response functions for an electron (plus positron) gas are written in terms of them. The dispersion is separated into Landau-damping, paircreation and dissipationless regimes. Explicit forms are given for the RQPDFs in the cases of a completely degenerate distribution and a nondegenerate thermal (Jüttner) distribution. Particular emphasis is placed on the relation between dissipation and dispersion, with the dissipation treated in terms of the imaginary parts of RQPDFs. Comparing the dissipation calculated in this way with the existing treatments leads to the identification of errors in the literature, which we correct. We also comment on a controversy as to whether the dispersion curves in a superdense plasma pass through the region where pair creation is allowed.

Dispersion relations in weakly degenerate plasmas

Spectrochimica Acta Part B: Atomic Spectroscopy, 2001

From a quantum mechanical point of view, electrons in laser produced plasmas can be regarded as weakly degenerate. For instance, for a plasma with electron density of 10 22 cm y3 and electron temperature of 1 eV, Sommerfeld's parameter is between 1 and 2. Under these conditions the usual dispersion relations for waves in plasmas need be corrected to account for degeneracy. In the present work, starting from the transport equation with a simplified version of the Boltzmann᎐Uehling᎐Uhlenbeck collision kernel the propagation of waves impinging on a plasma with weakly degenerate electrons is investigated and dispersion relations accounting for degeneracy are derived. These dispersion relations give the classical ones in the limit for Sommerfeld's parameter approaching zero. A shift of the wavenumber value and a non-collisional damping due to degeneracy effects are predicted which render a weakly degenerate plasma more opaque to radiation than a non-degenerate one. ᮊ

Plasma Dispersion Relations of Weakly and Non- Degenerate States

2015

Abstract: Condition for degeneracy of plasma by using the parameters density and temperature for different kinds of plasma were analysed on the basis of Sommerfield equation. Electrons in a laser produced plasma is considered as a weakly degenerate plasma.Dispersion relations are analyzed and studied.

An Introduction to Quantum Plasmas

Brazilian Journal of Physics, 2011

Shielding effects in non-degenerate and degenerate plasmas are compared. A detailed derivation of the Wigner-Poisson system is provided for electrostatic quantum plasmas in which relativistic, spin, and collisional effects are not essential. A detailed derivation of a quantum hydrodynamic model starting from the Wigner-Poisson system is presented. The route for this derivation considers the eikonal decomposition of the one-body wavefunctions of the quantum statistical mixture. The merits and limitations of the resulting quantum hydrodynamic model are discussed.

Monte Carlo simulations of dense quantum plasmas

Journal of Physics A: Mathematical and General, 2006

Thermodynamic properties of the equilibrium strongly coupled quantum plasmas investigated by direct path integral Monte Carlo (DPIMC) simulations within a wide region of density, temperature and positive to negative particle mass ratio. Pair distribution functions (PDF), equation of state (EOS), internal energy and Hugoniot are compared with available theoretical and experimental results. Possibilities of the phase transition in hydrogen and electron-hole plasma from neutral particle system to metallic-like state and crystal-like structures, including antiferromagnetic hole structure in semiconductors at low temperatures, are discussed.

Quantum Effects on the Linear Dispersion Characteristics in Electron-Positron Plasma

Journal of Nuclear Physics, Material Sciences, Radiation and Applications, 2014

In electron-positron plasmas some of the plasma modes are decoupled due to the equal charge to mass ratio of both species. The dispersion properties of the propagation of linear waves in degenerate electron-positron magnetoplasma are investigated. By using the quantum hydrodynamic equations with magnetic fields of the Wigner-Maxwell system, we have obtained a set of new dispersion relations in which ions' motions are not considered. The general dielectric tensor is derived using the electron and positron densities and its momentum response to the quantum effects due to Bohm potential and the statistical effect of Femi temperature. It has been demonstrated the importance of magnetic field and its role with the quantum effects in these plasmas which support the propagation of electromagnetic linear waves. Besides, the dispersion relations in case of parallel and perpendicular modes are investigated for different positron-electron density ratios.

Kinetic and correlation energies and distribution functions of dense plasmas

Physical Review E, 2002

The mean value of the kinetic energy of a quantum plasma is investigated in Hartree-Fock and Montroll-Ward approximations using the method of thermodynamic Green's functions. Usually, one finds the kinetic energy to be larger than that of an ideal plasma due to the interaction between the particles in the system. However, also the opposite case is possible, i.e., a decrease of the kinetic energy compared to that of the ideal gas. This special correlation effect is found for temperatures of about 10 6 K and densities between 10 21 and 10 26 cm Ϫ3. Here, the single-particle distribution function is shifted towards smaller momenta, and the binary distribution is changed.

Quantum Effects on Low Frequency Waves in Dense Plasmas

2009

This work is submitted as a dissertation in partial fulfillment of the requirements for the degree of DOCTOR OF PHILOSOPHY IN PHYSICS in the D e p a r t m e n t o f P h y s i c s COMSATS Institute of Information Technology I s l a m a b a d P a k i s t a n A u g u s t 2 0 0 9 This work is supported by Higher Education Commission (HEC) Pakistan under Indigenous PhD Fellowship Program (5000): No. 1751(P149)/HEC/Sch/2004

Effects of quantum statistical pressure and exchange correlation on the low frequency electromagnetic waves in degenerate Fermi-Dirac pair-ion plasma

arXiv: Plasma Physics, 2017

The low frequency, long wavelength electromagnetic waves, viz, shear Alfven wave in quantum electron-positron-ion magneto plasmas, have been examined using quantum magneto hydrodynamic model. In this model, we have considered electrons and positrons are to be magnetized as well as degenerate whereas ions are magnetized but classical. We have also included the effects of exchange correlation terms which appear entirely the dynamic equations of electrons and positrons. The whole treatment is done using multi-fluid model. Our object is to study the shear Alfv\'en waves propagating in above said system of plasma. For that we have derived the modified dispersion relation of the shear Alfv\'en waves. Results are relevant to the terrestrial laboratory astrophysics.

Dispersion relations in ultradegenerate relativistic plasmas

Physical Review D, 2000

The propagation of excitation modes in a relativistic ultradegenerate plasma is modified by their interactions with the medium. These modifications can be computed by evaluating their on-shell self-energy, which gives (gaugeindependent) dispersion relations. For modes with momentum close to the Fermi momentum, the one-loop fermion self-energy is dominated by a diagram with a soft photon in the loop. We find the one-loop dispersion relations for quasiparticles and antiquasiparticles, which behave differently as a consequence of their very different phase-space restrictions when they scatter with the electrons of the Fermi sea. In a relativistic system, the unscreened magnetic interactions spoil the normal Fermi liquid behavior of the plasma. For small values of the Fermi velocity, we recover the non-relativistic dispersion relations of condensed matter systems.