High and low frequency instabilities driven by counter-streaming electron beams in space plasmas

A four-component plasma composed of a drifting (parallel to ambient magnetic field) population of warm electrons, drifting (anti-parallel to ambient magnetic field) cool electrons, stationary hot electrons, and thermal ions is studied in an attempt to further our understanding of the excitation mechanisms of broadband electrostatic noise (BEN) in the Earth's magnetospheric regions such as the magnetosheath, plasmasphere, and plasma sheet boundary layer (PSBL). Using kinetic theory, beam-driven electrostatic instabilities such as the ion-acoustic, electron-acoustic instabilities are found to be supported in our multi-component model. The dependence of the instability growth rates and real frequencies on various plasma parameters such as beam speed, number density, temperature, and temperature anisotropy of the counter-streaming (relative to ambient magnetic field) cool electron beam are investigated. It is found that the number density of the anti-field aligned cool electron beam and drift speed play a central role in determining which instability is excited. Using plasma parameters which are closely correlated with the measurements made by the Cluster satellites in the PSBL region, we find that the electron-acoustic and ion-acoustic instabilities could account for the generation of BEN in this region.

[1]  R. Bharuthram,et al.  High and low frequency instabilities driven by a single electron beam in two-electron temperature space plasmas , 2013 .

[2]  G. Parks,et al.  Counterstreaming beams and flat-top electron distributions observed with Langmuir, Whistler, and compressional Alfvén waves in earth's magnetic tail. , 2008, Physical review letters.

[3]  X. Dou,et al.  Electrostatic waves in an electron-beam plasma system , 2005 .

[4]  Q. Lu,et al.  Generation mechanism of electrostatic solitary structures in the Earth's auroral region , 2005 .

[5]  R. Mace,et al.  The magnetized electron-acoustic instability driven by a warm, field-aligned electron beam , 2004 .

[6]  M. Hellberg,et al.  The Korteweg–de Vries–Zakharov–Kuznetsov equation for electron-acoustic waves , 2001 .

[7]  G. Lakhina,et al.  Generation of electron-acoustic waves in the magnetosphere , 2001 .

[8]  M. Hellberg,et al.  Electron-acoustic waves in the laboratory: an experiment revisited , 2000, Journal of Plasma Physics.

[9]  R. Treumann,et al.  Modulated electron‐acoustic waves in auroral density cavities: FAST observations , 1999 .

[10]  R. Treumann,et al.  Impulsive broadband electrostatic noise in the cleft: A signature of dayside reconnection , 1998 .

[11]  H. Matsumoto,et al.  Geotail waveform observations of broadband/narrowband electrostatic noise in the distant tail , 1997 .

[12]  M. Hellberg,et al.  On the existence of weak stationary electron-acoustic double layers , 1993, Journal of Plasma Physics.

[13]  M. Hellberg,et al.  Electron-acoustic and cyclotron-sound instabilities driven by field-aligned hot-electron streaming , 1993 .

[14]  R. Bharuthram Electron-acoustic instability driven by a field-aligned hot electron beam , 1991, Journal of Plasma Physics.

[15]  S. Baboolal,et al.  Arbitrary-amplitude electron-acoustic solitons in a two-electron-component plasma , 1991, Journal of Plasma Physics.

[16]  M. Ashour‐Abdalla,et al.  Injection of an overdense electron beam in space , 1990 .

[17]  S. Baboolal,et al.  Cut-off conditions and existence domains for large-amplitude ion-acoustic solitons and double layers in fluid plasmas , 1990, Journal of Plasma Physics.

[18]  C. Grabbe Wave propagation effects of broadband electrostatic noise in the magnetotail , 1989 .

[19]  M. Ashour‐Abdalla,et al.  Broadband electrostatic noise due to field-aligned currents , 1989 .

[20]  M. Ashour‐Abdalla,et al.  Generation of high-frequency broadband electrostatic noise: The role of cold electrons , 1987 .

[21]  C. Grabbe Numerical study of the spectrum of broadband electrostatic noise in the magnetotail , 1987 .

[22]  P. Shukla,et al.  Large amplitude ion‐acoustic double layers in a double Maxwellian electron plasma , 1986 .

[23]  M. Ashour‐Abdalla,et al.  Theory and simulations of broadband electrostatic noise in the geomagnetic tail , 1986 .

[24]  E. W. Hones,et al.  ISEE observations of the plasma sheet boundary, plasma sheet, and neutral sheet: 2. Waves , 1986 .

[25]  N. Omidi,et al.  The generation of broadband electrostatic noise by an ion beam in the magnetotail , 1986 .

[26]  Robert L. Tokar,et al.  The electron‐acoustic mode , 1985 .

[27]  Robert L. Tokar,et al.  Electrostatic hiss and the beam driven electron acoustic instability in the dayside polar cusp , 1984 .

[28]  T. Eastman,et al.  Generation of broadband electrostatic noise by ion beam instabilities in the magnetotail , 1983 .

[29]  D. Gurnett,et al.  Plasma waves in the distant magnetotail , 1976 .

[30]  Burton D. Fried,et al.  The Plasma Dispersion Function , 1961 .