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Prog. Theor. Phys. Vol. 49 No. 5 (1973) pp. 1483-1502

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Singlet Ground State of the Localized d-Electrons Coupled with Conduction Electrons in Metals

Isamu Okada and Kei Yosida

Institute for Solid State Physics, University of Tokyo, Roppongi, Tokyo

(Received December 23, 1972)

Abstract:

The theory of the singlet ground state for the s-d exchange model is extended to the core of d-electrons with orbital degeneracy. The effective s-d Hamiltonian is derived from the extended Anderson Hamiltonian by the Schrieffer-Wolff canonical transformation. On the basis of the effective Hamiltonian, the ground-state wave function and the ground-state energy are calculated. The anomalous part of the ground-state energy is given by -Dexp[N/(2l+1)ρJ], independently of the d-electron number, when the Hund coupling is neglected compared with the effective s-d interaction. This binding energy is much larger than that for a localized s-electron because of an extra factor of 1/(2l+1) in the exponent. This large value is caused mainly by the orbital quenching. For a more realistic case in which the Hund coupling is larger than the s-d interaction, it reduces to a smaller value of -Dexp[(2l+1)NJ] for a half-filled shell in which orbital exchange does not exist. This value is due purely to the spin quenching. Qualitative discussion is given about the spin quenching and orbital quenching on the effective Hamiltonian derived for n=2l, n being the number of d-electrons.


URL : http://ptp.ipap.jp/link?PTP/49/1483/
DOI : 10.1143/PTP.49.1483

[ Full Text PDF : FREE ACCESS (1443K) ] Citation:


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  12. Progress of Theoretical Physics Vol. 54 No. 4 (1975) pp. 967-981 :
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  14. Progress of Theoretical Physics Vol. 77 No. 5 (1987) pp. 1097-1115 :
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