Abstract
The electric field above the cathode surface of an Ar hollow cathode discharge has been measured by optogalvanic Stark spectroscopy. The field depends on the radial position of illumination and describes the radial distribution of the space charge density, ρ(r), as ρ(r) = –Ar + B, where r is the radial position and the parameters A and B are positive. The values of A and B increase with the discharge current, but the width of the cathode fall region remains nearly constant at about 1.02 ± 0.03 mm for a brass cathode of 5 mm i. d.
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References
1.
Little
P. F.
and
von Engel
A.
, Proc. Roy. Soc. London A224 , 209 (1954 ).
2.
Lidsky
L. M.
Rothleder
S. D.
Rose
D. J.
Yoshikawa
S.
Michelson
C.
, and
Mackin
R. J.
Jr.
, J. Appl. Phys. 33 , 2490 (1962 ).
3.
Sturges
D. J.
and
Oskam
H. J.
, J. Appl. Phys. 35 , 2887 (1964 ).
4.
Delcroix
J. L.
and
Trindade
A. R.
, Advances in Electronics and Electron Physics 35 , 87 (1974 ).
5.
Ingold
J. H.
, in Gaseous Electronics, Vol. 1, Electrical Discharge ,
Hirsh
M. N.
and
Oskam
H. J.
, Eds. (Academic Press , New York , 1978 ), Chap. 2.
6.
Nakajima
T.
Uchitomi
N.
Adachi
Y.
Maeda
S.
, and
Hirose
C.
, J. de Phys. Paris 44(C7) , 497 (1983 ).
7.
Fujimaki
S.
Adachi
Y.
, and
Hirose
C.
, Appl. Spectrosc. 41 , 567 (1987 ).
8.
Foster
J. S.
and
Horton
C. H.
, Phyl. Trans. Roy. Soc. 236A , 473 (1938 ).
9.
Masaki
T.
Wada
A.
Adachi
Y.
, and
Hirose
C.
, Appl. Spectrosc. 42 , 51 (1988 ).
