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Physical Mechanisms of the Electron Energy Distribution Function Control in Inhomogeneous Non-stationary Plasma. / Kudryavtsev, Anatoly; Tsendin, Lev.

In: Bulletin of the American Physical Society, Vol. 56, No. 15, 2011, p. 1.

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Harvard

Kudryavtsev, A & Tsendin, L 2011, 'Physical Mechanisms of the Electron Energy Distribution Function Control in Inhomogeneous Non-stationary Plasma', Bulletin of the American Physical Society, vol. 56, no. 15, pp. 1. <http://meetings.aps.org/link/BAPS.2011.GEC.AM1.11>

APA

Kudryavtsev, A., & Tsendin, L. (2011). Physical Mechanisms of the Electron Energy Distribution Function Control in Inhomogeneous Non-stationary Plasma. Bulletin of the American Physical Society, 56(15), 1. http://meetings.aps.org/link/BAPS.2011.GEC.AM1.11

Vancouver

Kudryavtsev A, Tsendin L. Physical Mechanisms of the Electron Energy Distribution Function Control in Inhomogeneous Non-stationary Plasma. Bulletin of the American Physical Society. 2011;56(15):1.

Author

Kudryavtsev, Anatoly ; Tsendin, Lev. / Physical Mechanisms of the Electron Energy Distribution Function Control in Inhomogeneous Non-stationary Plasma. In: Bulletin of the American Physical Society. 2011 ; Vol. 56, No. 15. pp. 1.

BibTeX

@article{fe9d67c7e0074bd8a7ee5f3570764bcf,
title = "Physical Mechanisms of the Electron Energy Distribution Function Control in Inhomogeneous Non-stationary Plasma",
abstract = "To predict the main scenarios of electron distribution function (EDF) control, first of all it is necessary to develop a kind of roadmap of formation a different modes of the EDF in the inhomogeneous unsteady plasma. The analysis shows that the time scales are determined by the ratio between the transient time tL (the characteristic time of electron transport through the plasma volume) and the relaxation times te of the EDF momentum tm (on velocity direction) and energy. Accordingly, for the spatial variable it is the ratio between the characteristic size of plasma L and an electron mean free path l (momentum relaxation) and a length of energy relaxation of electron energy le. A significant difference between the scale of momentum relaxation and energy te $>>$ tm, le $>>$ l (reaching two or more orders of magnitude), allows to predict the possible modes of the EDF formation, with various degrees of selectivity effects on different groups of electrons (from a local EDF when L $>>$ le and it is possible to affe",
author = "Anatoly Kudryavtsev and Lev Tsendin",
year = "2011",
language = "English",
volume = "56",
pages = "1",
journal = "Bulletin of the American Physical Society",
issn = "0003-0503",
publisher = "American Physical Society",
number = "15",

}

RIS

TY - JOUR

T1 - Physical Mechanisms of the Electron Energy Distribution Function Control in Inhomogeneous Non-stationary Plasma

AU - Kudryavtsev, Anatoly

AU - Tsendin, Lev

PY - 2011

Y1 - 2011

N2 - To predict the main scenarios of electron distribution function (EDF) control, first of all it is necessary to develop a kind of roadmap of formation a different modes of the EDF in the inhomogeneous unsteady plasma. The analysis shows that the time scales are determined by the ratio between the transient time tL (the characteristic time of electron transport through the plasma volume) and the relaxation times te of the EDF momentum tm (on velocity direction) and energy. Accordingly, for the spatial variable it is the ratio between the characteristic size of plasma L and an electron mean free path l (momentum relaxation) and a length of energy relaxation of electron energy le. A significant difference between the scale of momentum relaxation and energy te $>>$ tm, le $>>$ l (reaching two or more orders of magnitude), allows to predict the possible modes of the EDF formation, with various degrees of selectivity effects on different groups of electrons (from a local EDF when L $>>$ le and it is possible to affe

AB - To predict the main scenarios of electron distribution function (EDF) control, first of all it is necessary to develop a kind of roadmap of formation a different modes of the EDF in the inhomogeneous unsteady plasma. The analysis shows that the time scales are determined by the ratio between the transient time tL (the characteristic time of electron transport through the plasma volume) and the relaxation times te of the EDF momentum tm (on velocity direction) and energy. Accordingly, for the spatial variable it is the ratio between the characteristic size of plasma L and an electron mean free path l (momentum relaxation) and a length of energy relaxation of electron energy le. A significant difference between the scale of momentum relaxation and energy te $>>$ tm, le $>>$ l (reaching two or more orders of magnitude), allows to predict the possible modes of the EDF formation, with various degrees of selectivity effects on different groups of electrons (from a local EDF when L $>>$ le and it is possible to affe

M3 - Article

VL - 56

SP - 1

JO - Bulletin of the American Physical Society

JF - Bulletin of the American Physical Society

SN - 0003-0503

IS - 15

ER -

ID: 5292516