-
5
-
-
0032654285
-
-
E. Kawamura, V. Vahedi, M. A. Lieberman, and C. K. Birdsall, Plasma Sources Sci. Technol. 8, R45 (1999).
-
(1999)
Plasma Sources Sci. Technol.
, vol.8
-
-
Kawamura, E.1
Vahedi, V.2
Lieberman, M.A.3
Birdsall, C.K.4
-
6
-
-
0002274529
-
-
D. Field, D. F. Klemperer, P. W. May, and Y. P. Song, J. Appl. Phys. 70, 82 (1991).
-
(1991)
J. Appl. Phys.
, vol.70
, pp. 82
-
-
Field, D.1
Klemperer, D.F.2
May, P.W.3
Song, Y.P.4
-
8
-
-
0001381888
-
-
P. A. Miller, G. A. Hebner, K. E. Greenberg, P. D. Pochan, and B. P. Aragon, J. Res. Natl. Inst. Stand. Technol. 100, 427 (1995).
-
(1995)
J. Res. Natl. Inst. Stand. Technol.
, vol.100
, pp. 427
-
-
Miller, P.A.1
Hebner, G.A.2
Greenberg, K.E.3
Pochan, P.D.4
Aragon, B.P.5
-
9
-
-
12144260012
-
-
Y. Wang, E. C. Benck, M. Misakian, M. Edamura, and J. K. Olthoff, J. Appl. Phys. 87, (2000).
-
(2000)
J. Appl. Phys.
, vol.87
-
-
Wang, Y.1
Benck, E.C.2
Misakian, M.3
Edamura, M.4
Olthoff, J.K.5
-
12
-
-
0004036361
-
-
Chemical Rubber, Boca Raton, FL
-
For a discussion of quasistatic fields in capacitively coupled plasmas, see, for example, Y. P. Raizer, M. N. Schneider, and N. A. Yatsenko, Radio-Frequency Capacitive Discharges (Chemical Rubber, Boca Raton, FL, 1995).
-
(1995)
Radio-Frequency Capacitive Discharges
-
-
Raizer, Y.P.1
Schneider, M.N.2
Yatsenko, N.A.3
-
14
-
-
85037448216
-
-
8
-
8
-
-
-
-
15
-
-
0001096326
-
-
M. Fivaz, S. Brunner, W. Schwarzenbach, A. A. Howling, and Ch. Hollenstein, Plasma Sources Sci. Technol. 4, 373 (1995).
-
(1995)
Plasma Sources Sci. Technol.
, vol.4
, pp. 373
-
-
Fivaz, M.1
Brunner, S.2
Schwarzenbach, W.3
Howling, A.A.4
Hollenstein, Ch.5
-
16
-
-
85037467163
-
-
note
-
s indicates the sheath width and d is related to the electric field associated with the presheath. Approximately the same interpretation can be given here if we think of the presheath region as extending far into the body of the plasma and that d does not completely characterize the presheath region.
-
-
-
-
17
-
-
85037463082
-
-
note
-
Because the plasma and the corresponding impedance continually changes during the pulsed excitation of the plasma, it is not possible for the matching network coupling the rf energy to the coil to be continually optimized. For the IED measurements reported in this article, the matching network was optimized for continuous excitation and the rf power value indicated is for the net power to the matching network driving the coil under continuous excitation.
-
-
-
-
18
-
-
85037458766
-
-
determined from Measurement of Optical Emissions from Argon Plasma at 2.66 Pa (private communication)
-
E. Benck, determined from measurement of optical emissions from argon plasma at 2.66 Pa (private communication).
-
-
-
Benck, E.1
-
19
-
-
85037488589
-
-
note
-
o (26 μm) were reduced further.
-
-
-
-
21
-
-
0003913846
-
-
Addison-Wesely, Reading, MA
-
F. W. Sears, Thermodynamics, The Kinetic Theory of Gases, and Statistical Mechanics (Addison-Wesely, Reading, MA. 1953).
-
(1953)
Thermodynamics, the Kinetic Theory of Gases, and Statistical Mechanics
-
-
Sears, F.W.1
-
23
-
-
0031186974
-
-
J. Johannes, T. Bartel, G. A. Hebner, and J. Woodworth, J. Electrochem. Soc. 144, 2448 (1997).
-
(1997)
J. Electrochem. Soc.
, vol.144
, pp. 2448
-
-
Johannes, J.1
Bartel, T.2
Hebner, G.A.3
Woodworth, J.4
|