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THOMSON SCATTERING DIAGNOSTICS OF LASER‐PRODUCED ALUMINUM PLASMAS
1.N. G. Basov and O. N. Krokhin, Zh. Eksperim. i Teor. Fiz. 46, 17 (1964)
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3.see also A. F. Haught, D. H. Polk, and W. J. Fader, Conference Proceedings, Novosibirsk, August 1968 (IAEA, Vienna, 1969); Vol. 1, p. 925.
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13.The scattering parameter where is the incident wavelength (6943 Å), is the electron Debye length, and θ is the scattering angle (90°). Since the ratio is indeterminate and only is evaluated by fitting the experimental points to the theoretical Thomson scattering curve. In such cases the electron density can only be determined independently by some other method, such as by Rayleigh scattering. See Ref. 9.
14.Typically the expansion velocity of the outermost boundary of the plasma is about (see Refs. 6 and 7).
15.Ralph R. Rudder and David R. Bach, J. Opt. Soc. Am. 53, 1260 (1968).
16.The possibility of the importance of collision broadening was originally suggested to the authors by H. Dreicer of Los Alamos (private communication, August 1969).
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