Interaction of biased electrodes and plasmas: sheaths, double layers, and fireballs
Biased electrodes are common components of plasma sources and diagnostics. The plasma–
electrode interaction is mediated by an intervening sheath structure that influences …
electrode interaction is mediated by an intervening sheath structure that influences …
RFEA measurements of high-energy electrons in a helicon plasma device with expanding magnetic field
N Gulbrandsen, Å Fredriksen - Frontiers in Physics, 2017 - frontiersin.org
In the inductively coupled plasma of the Njord helicon device we have, for the same
parameters as for which an ion beam exists, measured a downstream population of high …
parameters as for which an ion beam exists, measured a downstream population of high …
Extensions and applications of the Bohm criterion
The generalized Bohm criterion is revisited in the context of incorporating kinetic effects of
the electron and ion distribution functions into the theory. The underlying assumptions and …
the electron and ion distribution functions into the theory. The underlying assumptions and …
Information hidden in the velocity distribution of ions and the exact kinetic Bohm criterion
TV Tsankov, U Czarnetzki - Plasma Sources Science and …, 2017 - iopscience.iop.org
Non-equilibrium distribution functions of electrons and ions play an important role in plasma
physics. A prominent example is the kinetic Bohm criterion. Since its first introduction it has …
physics. A prominent example is the kinetic Bohm criterion. Since its first introduction it has …
A comparison of ion beam measurements by retarding field energy analyzer and laser induced fluorescence in helicon plasma devices
Both Laser-Induced Fluorescence (LIF) and Retarding Field Energy Analyzers (RFEA) have
been applied to the investigation of beams formed in inductively coupled helicon plasmas …
been applied to the investigation of beams formed in inductively coupled helicon plasmas …
Numerical simulations of a sounding rocket in ionospheric plasma: Effects of magnetic field on the wake formation and rocket potential
D Darian, S Marholm, JJP Paulsson… - Journal of …, 2017 - Wiley Online Library
The charging of a sounding rocket in subsonic and supersonic plasma flows with external
magnetic field is studied with numerical particle‐in‐cell (PIC) simulations. A weakly …
magnetic field is studied with numerical particle‐in‐cell (PIC) simulations. A weakly …
Simulations of several finite-sized objects in plasma
WJ Miloch - Procedia Computer Science, 2015 - Elsevier
Interaction of plasma with finite-sized objects is one of central problems in the physics of
plas-mas. Since object charging is often nonlinear and involved, it is advisable to address …
plas-mas. Since object charging is often nonlinear and involved, it is advisable to address …
Examination of argon metastable atom velocity distribution function close to a conducting wall
N Claire, S Mazouffre, C Rebont, F Doveil - Physics of Plasmas, 2012 - pubs.aip.org
The spatial evolution of the 1 s 5 metastable argon atom velocity distribution function is
recorded in the sheath and pre-sheath regions of a metallic wall using laser induced …
recorded in the sheath and pre-sheath regions of a metallic wall using laser induced …
Sheath formation time for spherical Langmuir probes
KM Kjølerbakken, WJ Miloch, K Røed - Journal of Plasma Physics, 2023 - cambridge.org
The formation time of the surrounding sheath of Langmuir probes in an ionospheric plasma
has been studied to better understand the constraints this puts on the sampling frequency of …
has been studied to better understand the constraints this puts on the sampling frequency of …
Reply to comment on 'Kinetic theory of the presheath and the Bohm criterion'
SD Baalrud, CC Hegna - Plasma Sources Science and …, 2012 - iopscience.iop.org
In his comment, Riemann defends the conventional kinetic Bohm criterion (KBC) on the
basis that the underlying approximations become rigorous in the limit λ D/l→ 0, where λ D is …
basis that the underlying approximations become rigorous in the limit λ D/l→ 0, where λ D is …