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  • 1
    Electronic Resource
    Electronic Resource
    Springer
    Annales geophysicae 14 (1996), S. 1-10 
    ISSN: 0992-7689
    Source: Springer Online Journal Archives 1860-2000
    Topics: Geosciences , Physics
    Notes: Abstract The electromagnetic proton cyclotron anisotropy instability is excited if the hot proton temperature anisotropy, T⊥h/T\mid\mid h, is sufficiently large compared to unity, where the subscript h denotes the hot protons and the perpendicular and parallel symbols denote directions relative to the background magnetic field. This instability is important in the outer magnetosphere because it has been shown to lead to an upper bound on T⊥h/T\mid\mid h and to cool iron heating. Here one-dimensional initial-value hybrid simulations with spatial variations in the direction of the background magnetic field are used to study this instability in a homogeneous plasma model which represents three ionic constituents of the outer magnetosphere: hot anisotropic protons, cool, initially isotropic protons, and cool, initially isotropic singly ionized helium. These simulations show that the presence of a tenuous helium component does not significantly change the scalings of either the hot proton anisotropy upper bound or the heating of the cool protons. The simulations also show that the helium ion heating rate increases with 〈beta〉\mid\midh in contrast to the cool proton energization which decreases with this parameter. The prediction of this homogeneous plasma model, therefore, for cool ions subject to heating by the proton cyclotron instability is that the observed ratio of cool helium temperature to cool proton temperature should increase as 〈beta〉\mid\midh increases.
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  • 2
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Physics of Plasmas 7 (2000), S. 448-456 
    ISSN: 1089-7674
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Electron/electron instabilities arise in collisionless plasmas when the electron velocity distribution consists of two distinct components with a sufficiently large relative drift speed between them. If the less dense beam component is not too tenuous and sufficiently fast, the electron/electron beam instability is excited over a relatively broad range of frequencies. This instability is often studied in the electrostatic limit, which is appropriate at ωe/|Ωe|(very-much-greater-than)1, where ωe is the electron plasma frequency and Ωe is the electron cyclotron frequency, but is not necessarily valid at ωe/|Ωe|∼1. Here linear Vlasov dispersion theory has been used and fully electromagnetic particle-in-cell simulations have been run in a spatially homogeneous, magnetized plasma model at βe(very-much-less-than)1 and 0.5 ≤ωe/|Ωe|≤4.0. Theory and simulations (run to times of order 100ωe−1) of the electron/electron beam instability show the growth of appreciable magnetic fluctuations at ωe/|Ωe|〈2; these waves bear right-hand elliptical magnetic polarization. The simulations reproduce the well-known slowing and heating of the beam; at ωe/|Ωe|〈1 this heating is predominantly parallel to the background magnetic field, but as ωe/|Ωe| becomes greater than unity the perpendicular heating of the beam increases. The simulations also demonstrate that, for ωe/|Ωe|∼1, electromagnetic fluctuations impart to the more dense electron core component significant heating perpendicular to the background magnetic field. © 2000 American Institute of Physics.
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  • 3
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Physics of Plasmas 6 (1999), S. 2607-2612 
    ISSN: 1089-7674
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Enhanced fluctuations from electromagnetic heat flux instabilities may, through wave-particle scattering, constrain the electron heat flux which flows parallel to the background magnetic field in the solar wind. A corollary of this hypothesis is that instability thresholds should correspond to observable bounds on the heat flux. Here plasma and magnetic field data from February and March 1995 of the Ulysses mission is analyzed in terms of the core/halo electron model to yield scaling relations of dimensionless electron parameters and empirical upper bounds on the dimensionless heat flux as functions of the core β. Use of these scaling relations in linear Vlasov theory for the whistler and Alfvén heat flux instabilities in homogeneous plasmas yields threshold conditions on the dimensionless heat flux which are also functions of the electron core β. The empirical bounds and the theoretical thresholds are similar and are therefore consistent with the hypothesis. © 1999 American Institute of Physics.
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  • 4
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Physics of Plasmas 1 (1994), S. 1676-1683 
    ISSN: 1089-7674
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The ions of the terrestrial magnetosheath are typically observed to have bi-Maxwellian velocity distributions with T⊥(approximately-greater-than)T(parallel), where ⊥ and (parallel) denote directions perpendicular and parallel to the background magnetic field. Observations of the highly compressed magnetosheath have demonstrated an inverse correlation between the proton temperature anisotropy and the proton parallel β. Hybrid computer simulations have shown that wave–particle scattering by the proton cyclotron anisotropy instability can yield similar correlations between these two parameters. Although these correlations are due to nonlinear plasma processes, they correspond to a threshold of this instability that can be determined from linear Vlasov theory. This proton anisotropy/β correlation represents a limited closure relation for anisotropic magnetohydrodynamic plasma models.
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  • 5
    Electronic Resource
    Electronic Resource
    New York, NY : American Institute of Physics (AIP)
    Physics of Fluids 4 (1992), S. 2964-2974 
    ISSN: 1089-7666
    Source: AIP Digital Archive
    Topics: Physics
    Notes: A second-order theory for electrostatic instabilities driven by counterstreaming ion beams is developed which describes momentum coupling and heating of the plasma via wave–particle interactions. Exchange rates between the waves and particles are derived, which are suitable for the fluid equations simulating microscopic effects on macroscopic scales. Using a fully kinetic simulation, the electrostatic ion cyclotron instability due to counterstreaming H+ beams has been simulated. A power spectrum from the kinetic simulation is used to evaluate second-order exchange rates. The calculated heating and momentum loss from second-order theory is compared to the numerical simulation.
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  • 6
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Physics of Fluids 31 (1988), S. 1554-1567 
    ISSN: 1089-7666
    Source: AIP Digital Archive
    Topics: Physics
    Notes: A two-dimensional electrostatic particle-in-cell code is used to simulate the thermal expansion of a cylindrical plasma across a uniform magnetic field. The simulations show that at early times (i.e., short compared to an ion gyroperiod), the plasma develops three characteristic regions: a charge neutral core surrounded by a negatively charged region (the electron charge layer), and an external halo composed only of ions (the ion charge layer). The radii of these non-neutral regions increase when either the electron plasma to electron cyclotron frequency ratio ωpe/||Ωe|| increases or when the electron to ion temperature ratio, Te/Ti, decreases. These simulations, which have been run with an ion-to-electron mass ratio of 100, show that the plasma develops structure as a result of the growth of a nonoscillatory instability in the electron charge layer. This structure exhibits growth times short compared to the ion gyroperiod, and wavelengths of the order of the ion gyroradius. The mode number of this structure increases with decreasing ωpe/||Ωe||, with increasing initial radius of the plasma relative to the electron Debye length, and with increasing Te/Ti. The linear theory of the lower hybrid drift instability, driven by the E×B and ∇n×B electron drift velocities, provides a good description of the parametric variation of the structure wavelength. It is therefore concluded that this instability is the most likely source of the structure observed in these simulations.
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  • 7
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Physics of Fluids 28 (1985), S. 2439-2441 
    ISSN: 1089-7666
    Source: AIP Digital Archive
    Topics: Physics
    Notes: This paper examines electrostatic modes in an unmagnetized, homogeneous, Vlasov plasma with three Maxwellian components: ions, hot electrons, and cool electrons. In such a plasma, the electron-acoustic mode with frequencies between the ion and electron plasma frequencies may propagate with light damping. The conditions that allow propagation of this mode, which is distinct from the well-known ion-acoustic and Langmuir waves, are given in detail; approximate necessary conditions are 10(approximately-less-than)Th/Tc and 0〈nc〈0.8ne, where the subscripts c, h, and e refer to the cool and hot electron components and the total electron population, respectively.
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  • 8
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Physics of Fluids 30 (1987), S. 2745-2749 
    ISSN: 1089-7666
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The electron acoustic wave becomes a normal mode of an unmagnetized collisionless plasma in the presence of two electron components with similar densities, but strongly disparate temperatures. The characteristic frequency of this mode is the plasma frequency of the cooler electron component. If these two electron components have a relative drift speed several times the thermal speed of the cooler component, the electron/electron acoustic instability may arise. This paper describes the parametric dependences of the threshold drift speed and maximum growth rate of this instability, and compares these with the same properties of the electron/ion acoustic instability. Under the condition of zero current, the electron/ion acoustic instability typically has the lower threshold drift speed, so that observation of the electron/electron acoustic instability is a strong indication of the presence of an electrical current in the plasma.
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  • 9
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Physics of Fluids 29 (1986), S. 531-535 
    ISSN: 1089-7666
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The linear theory of electromagnetic instabilities at propagation parallel or antiparallel to a uniform magnetic field B(0) is used to calculate the relative phase angle ψj between the fluctuating velocity vector of the jth component and the fluctuating magnetic field. A criterion that determines when this phase relationship leads to observable gyrophase bunching during the linear growth phase of an instability is also derived. The theory is applied to bunching of ion components by ion beam instabilities. Among the electromagnetic cool ion beam instabilities, it is found that the right-hand resonant mode is most likely to cause observable gyrophase bunching of an ion beam during linear growth, and that for sufficiently large beam–core relative drift speeds, ψb (approximately-equal-to)90° at maximum growth for instability propagation parallel to B(0).
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  • 10
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Physics of Fluids 29 (1986), S. 4085-4090 
    ISSN: 1089-7666
    Source: AIP Digital Archive
    Topics: Physics
    Notes: This paper examines the linear theory of electrostatic waves and instabilities in an unmagnetized, homogeneous Vlasov plasma. The first configuration considered is that of a stable plasma with three Maxwellian components: electrons, positive ions, and negative ions. The dispersion properties of the lightly damped ion modes are studied as a function of relative electron density and relative component temperatures. The second configuration considered is that of a tenuous electron–ion beam with drift speed v0b streaming through a negative/positive ion plasma. If the beam is very tenuous, an electron beam instability satisfying ωr(approximately-equal-to)kv0b is excited; if the beam is more dense, the instability becomes Buneman-like with parabolic dispersion. The thresholds and maximum growth rates of these instabilities are described as functions of the beam density and drift speed.
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