IShTAR (Ion cyclotron Sheath Test ARrangement) is a linear magnetised plasma test facility for RF sheaths studies at the Max-Planck-Institut für Plasmaphysik in Garching. In contrast to a tokamak, a test stand provides more liberty to impose the parameters and gives better access for the instrumentation and antennas. The project will support the development of diagnostic methods for characterising RF sheaths and validate and improve theoretical predictions. The cylindrical vacuum vessel has a diameter of 1 m and is 1.1 m long. The plasma is created by an external cylindrical plasma source equipped with a helical antenna that has been designed to excite the m=1 helicon mode. In inductive mode, plasma densities and electron temperatures have been characterised with a planar Langmuir probe as a function of gas pressure and input RF power. A 2D array of RF compensated Langmuir probes and a spectrometer are planned. A single strap RF antenna has been designed; the plasma-facing surface is aligned to the cylindrical plasma to ease the modelling. The probes will allow direct measurements of plasma density profiles in front of the RF antenna, and thus a detailed study of the density modifications induced by RF sheaths, which influences the coupling. The RF antenna frequency has been chosen to study different plasma wave interactions: the accessible plasma density range includes an evanescent and propagative behaviour of slow or fast waves, and allows the study of the effect of the lower hybrid resonance layer.

1.
R.
D’Inca
,
K.
Crombé
 et al, “
IShTAR: a test facility to investigate sheath effects during Ion Cyclotron Reso-nance Heating
”,
in preparation
2.
R.
D’Inca
,
J.
Jacquot
 et al, “
First experimental results on the IShTAR testbed
”, this conference
3.
F.
Louche
,
J.
Jacquot
 et al, “
Designing the IShTAR antenna: physics and engineering aspects
”, this conference
4.
CST STUDIO SUITE
, CST AG, Germany, www.cst.com
5.
Comsol Multiphysics, www.comsol.com
6.
K.
Crombé
,
J.
Jacquot
,
F.
Louche
and
D.
Van Eester
, “
Numerical challenges in modelling near-antenna field behaviour in cold plasmas
”,
Proceedings of the 41st EPS Conference on Plasma Physics
,
23rd - 27th June 2014
,
Berlin, Germany
,
ECA
, Vol.
38F
(
2014
), P1.
039
7.
L.
Lu
 et al, “
Wave coupling in the magnetized plasma edge: impact of a finite, inhomogeneous density inside the antenna box
”, this conference
8.
K.
Crombé
and
D.
Van Eester
, “
Coupled and decoupled solutions of the cold plasma dispersion relation
”, in preparation
9.
T.H.
Stix
. “
Waves in Plasmas
”,
AIP
,
New York
(
1992
)
10.
D.
Van Eester
,
K.
Crombé
and
V.
Kyrytsya
,
Plasma Phys. Control. Fusion
55
(
2013
)
025002
11.
D.
Van Eester
,
K.
Crombé
and
V.
Kyrytsya
,
Plasma Phys. Control. Fusion
55
(
2013
)
055001
12.
T.
Wauters
 et al,
Plasma Physics and Controlled Fusion
53
(
2011
)
125003
.
13.
L.
Colas
 et al,
Phys. Plasmas
19
(
2012
)
092505
14.
J.
Jacquot
 et al,
Phys. Plasmas
21
(
2014
)
061509
15.
A.
Ngadjeu
,
E.
Faudot
,
J.
Gunn
,
L.
Colas
and
S.
Heuraux
,
AIP Conf. Proc.
1187
,
161
(
2009
)
16.
D.
Van Eester
,
K.
Crombé
and
L.
Lu
, “
Wave induced density modification in RF sheaths and close to wave launchers
”, this conference
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