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Numéro
J. Phys. I France
Volume 2, Numéro 4, April 1992
Page(s) 459 - 486
DOI https://doi.org/10.1051/jp1:1992157
References of J. Phys. I France 2 459-486
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  8. According to our definition of the Kondo temperature: T0 = J(J+1)g3j$\mu$2B/3kB$\chi$(0) where $\chi$(0) is the magnetic susceptibility at T = 0 K, and J = 7/2 and gj = 8/7 for Yb3+, the T0 of reference [7] is bigger titan ours by a factor 4$\pi$/(2J + 1) = 1.57.
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  12. The C constant for 170Yb3+ has been determined from the precise measurement of the hyperfine constant associated with the $\Gamma_{7}$ state for Yb3+ impurities in metallic and insulating hosts (see Bonville P., Imbert P., Jhanno G., Gonzalez-Jimenez F., Hartmann-Boutron F. Phys. Rev. B 30 (1984) 3672). The found value is: A( $\Gamma_{7}$) = (893 $\pm$ 5)MHz, hence C = $\frac{A(\Gamma_{7})} {g( \Gamma_{7})g_{n}\mu_{n}}$ = (102 $\pm$ 3) T/$\mu_{B}$.
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