A new type of in-vessel Penning gauge, the Wisconsin In Situ Penning (WISP) gauge, has been developed and successfully operated in the Wendelstein 7-X (W7-X) island divertor baffle and vacuum vessel. The capacity of the quantitative measurements of the neutral reservoir for light impurities, in particular, helium, is important for tokamaks as well as stellarator divertors in order to avoid fuel dilution and radiative energy loss. Penning gauges assisted by spectroscopy are a powerful tool to obtain the total neutral pressure as well as fractional neutral pressures of specific impurities. The WISP gauge is a miniaturized Penning gauge arrangement, which exploits the ambient magnetic field of magnetic confinement fusion experiments to establish the Penning discharge. Then, in situ spectroscopy is conducted to separate the fractional neutral pressures of hydrogen, helium, and possibly also other impurities. The WISP probe head was qualified using the magnetic field of the Magnetized Dusty Plasma Experiment at Auburn University between 0.25 T and 3.5 T [E. Thomas et al., J. Plasma Phys. 81, 345810206 (2015)]. The in-depth quantitative evaluation for hydrogen and helium will be shown as well as an exploration of nitrogen, argon, and neon. A power law scaling between current I and pressure p, I = f(Gas,V) · pn(Gas, B), was shown. The factor f is gas and anode potential dependent, while n is gas and magnetic field strength dependent. Pressure measurements from 0.1 mbar and down to 1 × 10−5 mbar were achieved, demonstrating a reliable operating range for relevant pressure levels in the divertor and main vessel regions in current and future fusion devices, with a time resolution of up to 1 kHz. The lowest achievable pressure measurement increases with an increase in B and can be shifted with the anode potential V. At W7-X, the WISP probe head was mounted on an immersion tube setup that passes through the cryostat and places the probe head close to the plasma. Two probe heads were positioned in different divertor pump gaps, top and bottom, and one close to the plasma on the midplane in one module. The gauges were in situ calibrated together with the ASDEX pressure gauges [G. Haas and H.-S. Bosch, Vacuum 51, 39 (1998)]. Data were taken during the entire operation phase 1.2b, and measurements were coherent with other neutral gas pressure gauges. For the spectroscopic partial pressure measurements, channels of a spectroscopic detection system based on photo-multipliers, a so-called filterscope [R. J. Colchin et al., Rev. Sci. Instrum. 74, 2068 (2003)], provided by the Oak Ridge National Lab were used.

1.
D.
Reiter
,
G. H.
Wolf
, and
H.
Kever
,
Nucl. Fusion
30
,
2141
(
1990
).
2.
K.
Ida
,
M.
Yoshinuma
,
B.
Wieland
,
M.
Goto
,
Y.
Nakamura
,
M.
Kobayashi
,
I.
Murakami
, and
C.
Moon
,
Rev. Sci. Instrum.
86
,
123514
(
2015
).
3.
A.
Kappatou
,
R. M.
McDermott
,
T.
Pütterich
,
R.
Dux
,
B.
Geiger
,
R. J. E.
Jaspers
,
A. J. H.
Donné
,
E.
Viezzer
,
M.
Cavedon
 et al.,
Plasma Phys. Controlled Fusion
60
,
055006
(
2018
).
4.
H.-S.
Bosch
,
G.
Haas
, and
M.
Lörcher
,
J. Nucl. Mater.
196-198
,
1074
(
1992
).
5.
K. H.
Finken
,
K. H.
Dippel
,
W. Y.
Baek
, and
A.
Hardtke
,
Rev. Sci. Instrum.
63
,
1
(
1992
).
7.
T.
Denner
,
K. H.
Finken
, and
G.
Mank
,
Rev. Sci. Instrum.
67
,
3515
(
1996
).
8.
M. R.
Wade
,
D. L.
Hillis
,
J. T.
Hogan
,
M. A.
Mahdavi
,
R.
Maingi
,
W. P.
West
,
N. H.
Brooks
,
K. H.
Burrell
,
R. J.
Groebner
,
G. L.
Jackson
 et al.,
Phys. Rev. Lett.
74
,
2702
(
1995
).
9.
D. L.
Hillis
,
C. C.
Klepper
,
M.
Von Hellermann
,
J.
Ehrenberg
,
K. H.
Finken
, and
G.
Mank
,
Fusion Eng. Des.
34-35
,
347
(
1997
).
10.
C. C.
Klepper
,
T. M.
Biewer
,
V. B.
Graves
,
P.
Andrew
,
P. C.
Lukens
,
C.
Marcus
,
M.
Shimada
,
S.
Hughes
,
B.
Boussier
,
D. W.
Johnson
 et al.,
Fusion Eng. Des.
96-97
,
803
(
2015
).
11.
K.
Flesch
,
T.
Kremeyer
,
O.
Schmitz
,
V.
Soukhanovskii
, and
U.
Wenzel
,
Rev. Sci. Instrum.
87
,
11E529
(
2016
).
12.
E.
Thomas
,
U.
Konopka
,
D.
Artis
,
B.
Lynch
,
S.
Leblanc
,
S.
Adams
,
R.
Merlino
, and
M.
Rosenberg
,
J. Plasma Phys.
81
,
345810206
(
2015
).
13.
H.
Saitoh
,
T. S.
Pedersen
,
U.
Hergenhahn
 et al.,
J. Phys.: Conf. Ser.
505
,
012045
(
2014
).
14.
O.
Schmitz
,
I. L.
Beigman
,
L. A.
Vainshtein
,
B.
Schweer
,
M.
Kantor
,
A.
Pospieszczyk
,
Y.
Xu
,
M.
Krychowiak
,
M.
Lehnen
,
U.
Samm
 et al.,
Plasma Phys. Controlled Fusion
50
,
115004
(
2008
).
15.
G. W.
Pacher
,
H. D.
Pacher
,
G.
Janeschitz
,
A. S.
Kukushkin
,
V.
Kotov
, and
D.
Reiter
,
Nucl. Fusion
47
,
469
(
2007
).
16.
D.
Douai
,
T.
Goodman
,
A.
Isayama
 et al.,
Nucl. Fusion
58
,
026018
(
2017
).
17.
C. C.
Klepper
,
D. L.
Hillis
,
M. R.
Wade
 et al.,
Rev. Sci. Instrum.
68
,
400
(
1997
).
18.
H.-S.
Bosch
,
R.
Brakel
,
T.
Braeuer
,
V.
Bykov
,
P.
van Eeten
,
J.-H.
Feist
,
F.
Füllenbach
,
M.
Gasparotto
,
H.
Grote
,
T.
Klinger
 et al.,
Nucl. Fusion
57
,
116015
(
2017
).
19.
U.
Wenzel
,
T.
Kremeyer
,
G.
Schlisio
,
M.
Marquardt
,
T. S.
Pedersen
,
O.
Schmitz
,
B.
Mackie
,
J.
Maisano-Brown
 et al.,
J. Instrum.
12
,
C09008
(
2017
).
20.
R. J.
Colchin
,
D. L.
Hillis
,
R.
Maingi
,
C. C.
Klepper
, and
N. H.
Brooks
,
Rev. Sci. Instrum.
74
,
2068
(
2003
).
21.
C. C.
Klepper
,
T. M.
Biewer
,
C.
Marcus
 et al.,
J. Instrum.
12
,
C10012
(
2017
).
22.
U.
Wenzel
,
T. S.
Pedersen
,
M.
Marquardt
, and
M.
Singer
,
Rev. Sci. Instrum.
89
,
033503
(
2018
).
23.
R.
Raman
,
H. W.
Kugel
,
T.
Provost
,
R.
Gernhardt
,
T. R.
Jarboe
, and
M. G.
Bell
,
Rev. Sci. Instrum.
74
,
1900
(
2003
).
24.
B.
Lipschultz
,
B.
LaBombard
,
C. S.
Pitcher
 et al.,
Plasma Phys. Controlled Fusion
44
,
733
(
2002
).
25.
B.
Boivin
, Report No. PSFC/RR-15-12,
2015
.
26.
G.
Haas
and
H.-S.
Bosch
,
Vacuum
51
,
39
(
1998
).
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