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Extra resources for ANSI-IEEE STD C57.98-1986 guide for transformer imp
1986); (d) Kasdan et al. (1975b); (e) Lewerenz et al. (1983); (f) Miller and Farley (1987), Al-Za'al et al. (1987); (g) Rosenbaum et al. (1986); (h) Werner et al. (1983); (i) Gruebele et al. (1987); (j) Senekowitsch et al. (1985); (k) Stevens Miller et al. (1987); (I) Stevens et al. (1983). X 3C-, u = 0 threshold. 15 ms. They identified the excited states as a 'A and X 'C-, v = 1, respectively, and the decay processes as the forbidden radiative transition a 'A + X 3X-,and the u = 1 + 0 infrared transition.
The dependence on u' is not marked (Rosmus and Werner). For u' 2 5, autodetachment occurs. The lifetimes toward this have been measured by Hefter et al. (1983). 0189 Source: After Mead et al. (1985). Note: Except for T,, which is in eV, and re, which is in A, the constants are in wave numbers. David R. 017 - Source: a is from Zeitz et al. (1979); b is from Rosmus and Werner (1984). Note: Except for T,, which is in eV, and re, which is in A, the constants are in wave numbers. decrease sharply as u' is increased and for u' 2 6 are much shorter than the radiative lifetimes.
Predicted binding energies less than Be are bracketed. Adamowicz and McCullough (1984b) found that taking electron correlation into account increased the calculated binding eV. 6 x 10-4 (3 x (6 x (5 x 10-8) 5 Source: After Adamowicz and McCullough (1984a). 6 x (5 x 10-8) 42 David R. Bates cause much error in the unbracketed values of Table XXII, but that the states having bracketed values are unbound with the possible exception of MgO (nl = 3). Adamowicz and Bartlett (1985, 1986a, 1988) have carried out more accurate BO approximation calculations on the first excited states of BeO-, LiF-, LiCl-, NaF-, and NaCl-.