Spectral Kinetic Simulation of the Ideal Multipole Resonance Probe

Publikation: Beiträge in ZeitschriftenKonferenz-Abstracts in FachzeitschriftenForschungbegutachtet

Standard

Spectral Kinetic Simulation of the Ideal Multipole Resonance Probe. / Gong, Junbo; Wilczek, Sebastian; Szeremley, Daniel et al.
in: Bulletin of the American Physical Society, Jahrgang 60, Nr. 9, 10.2015.

Publikation: Beiträge in ZeitschriftenKonferenz-Abstracts in FachzeitschriftenForschungbegutachtet

Harvard

Gong, J, Wilczek, S, Szeremley, D, Oberrath, J, Eremin, D, Dobrygin, W, Schilling, C, Friedrichs, M & Brinkmann, RP 2015, 'Spectral Kinetic Simulation of the Ideal Multipole Resonance Probe', Bulletin of the American Physical Society, Jg. 60, Nr. 9. <http://meetings.aps.org/Meeting/GEC15/Session/GT1.101>

APA

Gong, J., Wilczek, S., Szeremley, D., Oberrath, J., Eremin, D., Dobrygin, W., Schilling, C., Friedrichs, M., & Brinkmann, R. P. (2015). Spectral Kinetic Simulation of the Ideal Multipole Resonance Probe. Bulletin of the American Physical Society, 60(9). http://meetings.aps.org/Meeting/GEC15/Session/GT1.101

Vancouver

Bibtex

@article{26f4496c3a0c4f868375a77bd8a72626,
title = "Spectral Kinetic Simulation of the Ideal Multipole Resonance Probe",
abstract = "The term Active Plasma Resonance Spectroscopy (APRS) denotes a class of diagnostic techniques which utilize the natural ability of plasmas to resonate on or near the electron plasma frequency ωpe: An RF signal in the GHz range is coupled into the plasma via an electric probe; the spectral response of the plasma is recorded, and a mathematical model is used to determine plasma parameters such as the electron density ne or the electron temperature Te. One particular realization of the method is the Multipole Resonance Probe (MRP). The ideal MRP is a geometrically simplified version of that probe; it consists of two dielectrically shielded, hemispherical electrodes to which the RF signal is applied. A particle-based numerical algorithm is described which enables a kinetic simulation of the interaction of the probe with the plasma. Similar to the well-known particlein-cell (PIC), it contains of two modules, a particle pusher and a field solver. The Poisson solver determines, with the help of a truncated expansion into spherical harmonics, the new electric field at each particle position directly without invoking a numerical grid. The effort of the scheme scales linearly with the ensemble size N.",
keywords = "Engineering",
author = "Junbo Gong and Sebastian Wilczek and Daniel Szeremley and Jens Oberrath and Denis Eremin and Wladislav Dobrygin and Christian Schilling and Michael Friedrichs and Brinkmann, {Ralf Peter}",
note = "68th Annual Gaseous Electronics Conference/9th International Conference on Reactive Plasmas/33rd Symposium on Plasma Processing, October 12–16, 2015; Honolulu, Hawaii. Abstract ID: BAPS.2015.GEC.GT1.101 ",
year = "2015",
month = oct,
language = "English",
volume = "60",
journal = "Bulletin of the American Physical Society",
issn = "0003-0503",
publisher = "American Physical Society",
number = "9",

}

RIS

TY - JOUR

T1 - Spectral Kinetic Simulation of the Ideal Multipole Resonance Probe

AU - Gong, Junbo

AU - Wilczek, Sebastian

AU - Szeremley, Daniel

AU - Oberrath, Jens

AU - Eremin, Denis

AU - Dobrygin, Wladislav

AU - Schilling, Christian

AU - Friedrichs, Michael

AU - Brinkmann, Ralf Peter

N1 - 68th Annual Gaseous Electronics Conference/9th International Conference on Reactive Plasmas/33rd Symposium on Plasma Processing, October 12–16, 2015; Honolulu, Hawaii. Abstract ID: BAPS.2015.GEC.GT1.101

PY - 2015/10

Y1 - 2015/10

N2 - The term Active Plasma Resonance Spectroscopy (APRS) denotes a class of diagnostic techniques which utilize the natural ability of plasmas to resonate on or near the electron plasma frequency ωpe: An RF signal in the GHz range is coupled into the plasma via an electric probe; the spectral response of the plasma is recorded, and a mathematical model is used to determine plasma parameters such as the electron density ne or the electron temperature Te. One particular realization of the method is the Multipole Resonance Probe (MRP). The ideal MRP is a geometrically simplified version of that probe; it consists of two dielectrically shielded, hemispherical electrodes to which the RF signal is applied. A particle-based numerical algorithm is described which enables a kinetic simulation of the interaction of the probe with the plasma. Similar to the well-known particlein-cell (PIC), it contains of two modules, a particle pusher and a field solver. The Poisson solver determines, with the help of a truncated expansion into spherical harmonics, the new electric field at each particle position directly without invoking a numerical grid. The effort of the scheme scales linearly with the ensemble size N.

AB - The term Active Plasma Resonance Spectroscopy (APRS) denotes a class of diagnostic techniques which utilize the natural ability of plasmas to resonate on or near the electron plasma frequency ωpe: An RF signal in the GHz range is coupled into the plasma via an electric probe; the spectral response of the plasma is recorded, and a mathematical model is used to determine plasma parameters such as the electron density ne or the electron temperature Te. One particular realization of the method is the Multipole Resonance Probe (MRP). The ideal MRP is a geometrically simplified version of that probe; it consists of two dielectrically shielded, hemispherical electrodes to which the RF signal is applied. A particle-based numerical algorithm is described which enables a kinetic simulation of the interaction of the probe with the plasma. Similar to the well-known particlein-cell (PIC), it contains of two modules, a particle pusher and a field solver. The Poisson solver determines, with the help of a truncated expansion into spherical harmonics, the new electric field at each particle position directly without invoking a numerical grid. The effort of the scheme scales linearly with the ensemble size N.

KW - Engineering

M3 - Conference abstract in journal

VL - 60

JO - Bulletin of the American Physical Society

JF - Bulletin of the American Physical Society

SN - 0003-0503

IS - 9

ER -

Links