-
3
-
-
84931518076
-
-
R. W. Crompton points out that r in Eqs. (2) and (3) should be replaced by ρ = | r vec | sin theta and that gr( v vec ) should be replaced by gρ( v vec ) in Eqs. (2)–(18). Here r vec remains unchanged. J. P. Novak points out that the units of w in Table I should be 104~ m ~ sec-1. Also, the left-hand side of Eq. (24) should be multiplied by N and the first factor on the right-hand side of the equation for wII after Eq. (23) should be eE/3N. The last two terms in Eq. (19) should be multiplied by j and j+1, respectively.
-
-
-
-
11
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-
84931518070
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-
(unpublished). Note the Kücükarpaci and Lucas find it necessary to reduce the vibrational excitation cross sections of Ref. 22 by a factor of 0.3. The use of such low cross sections in our calculation gives a very poor fit to experiment, e.g., a factor of about 4 error in the energy-exchange frequency of Ref. 22 for mean electron energies near 1 eV.
-
-
-
Kunhardt, E.E.1
Tzeng, Y.2
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22
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-
4243200584
-
-
Consider the form of this technique described by
-
(1959)
Z. Phys.
, vol.156
, pp. 144
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-
Frommhold, L.1
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23
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-
84931518071
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-
During the current growth portion of the waveform the voltage is given by (Q0/ C) exp(ν t), where Q0 is the charge released from the cathode and C is the circuit capacity. After the electrons and ions have been collected the voltage is given by (Q0/ C)exp(αid). From the time of intersection of these curves we find d/t= ν / αi= Vp.
-
-
-
-
42
-
-
84931518068
-
-
Note that the value from Bromberg has been reinterpreted as discussed by Finn and Doering.
-
-
-
-
45
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-
84931521531
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-
The magnitudes of the spherical-harmonic components of the screened Coulomb cross sections were calculated using formulas given by, edited by, B. Alder, S. Fernbach, M. Rotenberg, Academic, New York, As suggested by these references, our comparisons of experiment and theory suggest screening lengths of 0.015 at 500 eV and 0.01 at 1 keV.
-
(1963)
Methods in Computational Physics
, pp. 209
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-
Berger, M.J.1
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46
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-
84931518084
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-
Nagoya Institute of Technology
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(1981)
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-
Hayashi, M.1
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49
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-
84982593791
-
Zur mikrophysikalischen Beschreibung des schwachionisierten Stickstoffmolekülplasmas der positiven Säule von Glimmentladungen. III. Elektronenkinetische Kenngrößen unter Berücksichtigung der Dissoziation durch direkten Elektronenstoß
-
(1978)
Beiträge aus der Plasmaphysik
, vol.18
, pp. 113
-
-
Pfau, S.1
Winkler, W.2
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54
-
-
84931518083
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-
U. S. National Aeronautics and Space Administration Technical Note No. TN-D-8347, 1976 (unpublished);
-
-
-
-
69
-
-
84931517871
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-
Joint Insitute for Laboratory Astrophysics Information Center, (unpublished). The data tabulated in this report were modified to give a common energy grid for all levels while preserving the areas under the peaks in the cross sections.
-
(1973)
-
-
Kieffer, L.J.1
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78
-
-
84931517870
-
-
For our purposes these changes are small and will be neglected.
-
-
-
-
94
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-
84931517869
-
-
The cross-section values actually used are from C. F. Barnet, J. A. Ray, E. Ricci, M. I. Wilker, E. W. McDaniel, E. W. Thomas, and H. B. Gilbody, Oak Ridge National Laboratory Report No. 5207, 1977 (unpublished).
-
-
-
-
101
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-
84931517868
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-
It should be kept in mind that the differential scattering cross sections reconstructed from our limited number of spherical harmonics will not give a good representation of a sharply peaked angular distribution at small scattering angles and may become negative at some large angles.
-
-
-
-
114
-
-
84931517867
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-
see also B. M. Penetrante, J. N. Bardsley, and L. C. Pitchford (unpublished).
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-
-
-
129
-
-
84931517866
-
-
See comment in the title of Fig. 2.6 of G. J. Schulz, in Principles of Laser Plasmas, edited by G. Bekefi (Wiley, New York, 1976), p. 47; see also, Jung et al. (Ref. 30).
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-
-
-
130
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-
4243177368
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-
For a recent review, see, P. Segur, edited by, E. E. Kunhardt, L. H. Luessen, Plenum, New York
-
(1981)
Electrical Breakdown and Discharges in Gases
, pp. 331
-
-
Yousfi, M.1
Bouef, J.P.2
Marode, E.3
Davies, A.J.4
Evans, J.G.5
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140
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-
36749117711
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-
It appears to us that the procedure of Lin, Robson, and Mason does not belong in this category, since they made the spherical-harmonic expansion before making the velocity-moment expansion. See
-
(1979)
J. Chem. Phys.
, vol.71
, pp. 3483
-
-
Lin, S.L.1
Robson, R.E.2
Mason, E.A.3
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155
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-
0017940890
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-
When the distribution of vibrationally excited molecules produced during the excitation period is used instead of the rate coefficients in Eq. (B1), we obtain the equivalent of the equation given in this reference.
-
(1978)
Sov. J. Plasma Phys.
, vol.4
, pp. 201
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-
-
160
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-
0001124879
-
-
(1982)
Teplofiz. Vys. Temp.
, vol.20
, pp. 818
-
-
Akishev, Yu. S.1
Dem'yanov, A.V.2
Kochetov, I.V.3
Napartovich, A.P.4
Pashkin, S.V.5
Ponomarenko, V.V.6
Pevgov, V.G.7
Podobedov, V.B.8
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