Power Transmission Factor for Tungsten Target w/wo Fiber-Form Nanostructure in He Plasmas with Hot Electron Component Using Compact Plasma Device AIT-PID

2013 ◽  
Vol 63 (1T) ◽  
pp. 225-228 ◽  
Author(s):  
S. Takamura ◽  
T. Miyamoto ◽  
N. Ohno
2011 ◽  
Vol 116 (A9) ◽  
pp. n/a-n/a ◽  
Author(s):  
K. Yoshioka ◽  
I. Yoshikawa ◽  
F. Tsuchiya ◽  
M. Kagitani ◽  
G. Murakami

1992 ◽  
Vol 196-198 ◽  
pp. 860-864 ◽  
Author(s):  
A.H. Futch ◽  
G.F. Matthews ◽  
D. Buchenauer ◽  
D.N. Hill ◽  
R.A. Jong ◽  
...  

2000 ◽  
Vol 64 (4) ◽  
pp. 433-443 ◽  
Author(s):  
M. A. HELLBERG ◽  
R. L. MACE ◽  
R. J. ARMSTRONG ◽  
G. KARLSTAD

High-frequency electrostatic waves have been observed in a two-electron-temperature plasma. Both bi-Maxwellian and Maxwellian-waterbag models were found to be inadequate in explaining the observed dispersion and damping rates. However, modelling of the hot electron component with a κ-distribution function confirms that the experiments represent observation of the electron-acoustic wave in the laboratory.


2009 ◽  
Vol 390-391 ◽  
pp. 839-842 ◽  
Author(s):  
J.G. Watkins ◽  
T.E. Evans ◽  
M. Jakubowski ◽  
R.A. Moyer ◽  
O. Schmitz ◽  
...  

1992 ◽  
Vol 47 (9) ◽  
pp. 935-940 ◽  
Author(s):  
N. Marinescu ◽  
M. Apostol

Abstract A Klein-Gordon-type equation is derived for the wave propagation in an ideal, uniform waveguide, and its quantum-mechanical interpretation is given. The "cross-section" concept is introduced for a waveguide and the power transmission factor is obtained by using standard methods of quantum mechanics. The spinorial formalism is also employed for deriving the equivalent Dirac-type equation, and the perturbation theory is applied for computing the frequency shifts. The general applicability of the quantum-mechanical concepts to the waveguides theory is discussed


1991 ◽  
Vol 45 (3) ◽  
pp. 323-338 ◽  
Author(s):  
R. L. Mace ◽  
S. Baboolal ◽  
R. Bharuthram ◽  
M. A. Hellberg

Motivated by plasma and wave measurements in the cusp auroral region, we have investigated electron-acoustic solitons in a plasma consisting of fluid ions, a cool fluid electron and a hot Boltzmann electron component. A recently described method of integrating the full nonlinear fluid equations as an initial-value problem is used to construct electron-acoustic solitons of arbitrary amplitude. Using the reductive perturbation technique, a Korteweg-de Vries equation, which includes the effects of finite cool-electron and ion temperatures, is derived, and results are compared with the full theory. Both theories admit rarefactive soliton solutions only. The solitons are found to propagate at speeds greater than the electron sound speed (ε0c/ε0ε)½υε, and their profiles are independent of ion parameters. It is found that the KdV theory is not a good approximation for intermediate-strength solitons. Nor does it exhibit the fact that the cool- to hot-electron temperature ratio restricts the parameter range over which electron-acoustic solitons may exist, as found in the arbitrary-amplitude calculations.


2020 ◽  
Author(s):  
Mika Holmberg ◽  
Fabrice Cipriani ◽  
Grégoire Déprez ◽  
Christian Imhof ◽  
Olivier Witasse ◽  
...  

<div class="x_gmail-co_mto_htmlabstract-content x_gmail-mt-3"> <p>We use Spacecraft Plasma Interaction Software (SPIS) simulations of the surface charging of the Jupiter Icy Moons Explorer (JUICE) spacecraft to study how the variable magnetospheric environment of Jupiter will impact the future JUICE particle and electric field measurements.</p> <p>The study has been limited to the magnetospheric region relevant for JUICE, that is, the environments of the inner and middle magnetosphere of Jupiter. The closest approach of Jupiter will be at 9.3 R<sub>J</sub>. In the inner magnetosphere the spacecraft will charge a few volts negative for the typical plasma sheet environment, where n<sub>e,cold</sub> ≈ 50 cm<sup>-3</sup> and T<sub>e,cold</sub> ≈ 20 eV. However, Galileo detected plasma densities of up to 600 cm<sup>-3</sup> in the region around 9.4 R<sub>J</sub> (Kurth et al., 2001). These densities could be due to activity on Europa, such as plumes, or a local disturbance of cold and dense iogenic plasma (Bagenal et al., 2015). Such high densities could result in surface potentials of tens of volts, when assuming T<sub>e,cold</sub> ≈ 5 eV, which would inhibit cold electron measurements performed by the electron spectrometer of JUICE, since the electrons would be repelled before reaching the detector. In addition, the large differential charging of tens of volts, due to the dielectric surfaces, would disturb electric field measurements. However, the cold electron temperature is not well constrained for this particular disturbance and a lower plasma temperatures would decrease the magnitude of the surface potential.</p> <p>Our SPIS simulations show surface potentials of a few volts positive for typical magnetospheric environments in the plasma sheet between 15 and 26 R<sub>J</sub>, where n<sub>e,cold</sub> > 20 n<sub>e,hot</sub> and the hot electron component range from 1-5 keV. However, Galileo measurements occasionally show hot electron densities equal to or slightly larger than the typical cold electron densities (Futaana et al., 2018). Simulated surface potentials, using n<sub>e,cold</sub> ≈ n<sub>e,hot</sub>, show no significant difference compared to the typical environment since the increase in hot electrons is counterbalanced by the increase in the production of secondary electrons. In this particular environment, higher electron densities will charge the spacecraft more negative while higher secondary electron production will charge the spacecraft more positive. Assuming Maxwellian distributions, we obtain that an unusually dense hot, 1-5 keV, electron component, like the one measured by Galileo, would not disturb the particle measurements of JUICE.</p> <p>Our study shows that the absolute charging of the spacecraft strongly depends on the cold electron density and temperature, and, for certain environments, on the spacecraft orientation relative to the plasma flow and the solar radiation. An unusually dense and hot, 1-5 keV, electron plasma component will not have a substantial impact on the charging, in the studied region. We are investigating whether different energy distributons will change this conclusion. The SPIS JUICE surface charging simulation results show that only minor perturbations will be obtained in typical Jovian magnetospheric environments, while substantial perturbations will occasionally occur in the disturbed magnetosphere.</p> </div>


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