An Improved Tabulation of the Plasma Dispersion Function and Its First Derivative--Part I: Argument with Positive Imaginary Part; Part II: Argument with Negative Imaginary Part: Zeros and Saddle Points

1973 ◽  
Vol 27 (124) ◽  
pp. 1002
Author(s):  
Y. L. L. ◽  
Henry E. Fettis ◽  
James C. Caslin ◽  
Kenneth R. Cramer
Keyword(s):  
Imaginary Part ◽  
Saddle Points ◽  
Dispersion Function ◽  
Positive Imaginary Part ◽  
First Derivative ◽  
Negative Imaginary Part ◽  
Plasma Dispersion

Expansions of the mildly relativistic dispersion function for nearly perpendicular electron cyclotron ray tracing

1999 ◽  
Vol 61 (1) ◽  
pp. 121-128 ◽  
Author(s):  
I. P. SHKAROFSKY
Keyword(s):  
Ray Tracing ◽  
Computer Programs ◽  
Higher Order ◽  
Electron Cyclotron ◽  
Dispersion Function ◽  
Relativistic Dispersion ◽  
Plasma Dispersion ◽  
Derivatives Of ◽  
Cyclotron Harmonic ◽  
Experienced Difficulty

To trace rays very close to the nth electron cyclotron harmonic, we need the mildly relativistic plasma dispersion function and its higher-order derivatives. Expressions for these functions have been obtained as an expansion for nearly perpendicular propagation in a region where computer programs have previously experienced difficulty in accuracy, namely when the magnitude of (c/vt)2 (ω−nωc)/ω is between 1 and 10. In this region, the large-argument expansions are not yet valid, but partial cancellations of terms occur. The expansion is expressed as a sum over derivatives of the ordinary dispersion function Z. New expressions are derived to relate higher-order derivatives of Z to Z itself in this region of concern in terms of a finite series.

Plasma dispersion function for a Fermi–Dirac distribution

2010 ◽  
Vol 17 (12) ◽  
pp. 122103 ◽  
Author(s):  
D. B. Melrose ◽  
A. Mushtaq
Keyword(s):  
Dispersion Function ◽  
Dirac Distribution ◽  
Plasma Dispersion

scholarly journals Electron velocity distribution function in a plasma with temperature gradient and in the presence of suprathermal electrons: application to incoherent-scatter plasma lines

1998 ◽  
Vol 16 (10) ◽  
pp. 1226-1240 ◽  
Author(s):  
P. Guio ◽  
J. Lilensten ◽  
W. Kofman ◽  
N. Bjørnå
Keyword(s):  
Distribution Function ◽  
Temperature Gradient ◽  
Velocity Distribution ◽  
Velocity Distribution Function ◽  
Electron Velocity ◽  
Dispersion Function ◽  
Electron Velocity Distribution ◽  
Incoherent Scatter ◽  
Suprathermal Electrons ◽  
Plasma Dispersion

Abstract. The plasma dispersion function and the reduced velocity distribution function are calculated numerically for any arbitrary velocity distribution function with cylindrical symmetry along the magnetic field. The electron velocity distribution is separated into two distributions representing the distribution of the ambient electrons and the suprathermal electrons. The velocity distribution function of the ambient electrons is modelled by a near-Maxwellian distribution function in presence of a temperature gradient and a potential electric field. The velocity distribution function of the suprathermal electrons is derived from a numerical model of the angular energy flux spectrum obtained by solving the transport equation of electrons. The numerical method used to calculate the plasma dispersion function and the reduced velocity distribution is described. The numerical code is used with simulated data to evaluate the Doppler frequency asymmetry between the up- and downshifted plasma lines of the incoherent-scatter plasma lines at different wave vectors. It is shown that the observed Doppler asymmetry is more dependent on deviation from the Maxwellian through the thermal part for high-frequency radars, while for low-frequency radars the Doppler asymmetry depends more on the presence of a suprathermal population. It is also seen that the full evaluation of the plasma dispersion function gives larger Doppler asymmetry than the heat flow approximation for Langmuir waves with phase velocity about three to six times the mean thermal velocity. For such waves the moment expansion of the dispersion function is not fully valid and the full calculation of the dispersion function is needed.Key words. Non-Maxwellian electron velocity distribution · Incoherent scatter plasma lines · EISCAT · Dielectric response function

Sign in / Sign up

Export Citation Format

Share Document