Magnetic field effects for the asymmetric Anderson Hamiltonian
- 1 December 1984
- journal article
- research article
- Published by American Physical Society (APS) in Physical Review B
- Vol. 30 (11), 6717-6731
- https://doi.org/10.1103/physrevb.30.6717
Abstract
Perturbation expansion for the asymmetric single-orbital Anderson Hamiltonian is extended to the case with finite magnetic field, and the self-energy part of the -electron Green function is calculated up to the second order in for arbitrary asymmetry and magnetic field . Zero-temperature density of localized states , magnetic moment and static spin susceptibility , and low-temperature specific heat and magnetoresistance of a dilute alloy are evaluated within the approximation. Plausible arguments are given (which become exact in the symmetric case) that the higher-order terms do not change the qualitative features of our results. For large enough the many-body (MB) effects give rise to three different types of behavior, depending on the value of asymmetry: (i) spin-fluctuation behavior for , with large fluctuations of the -level magnetization; (ii) mixed-valence behavior for , with large fluctuations of the -level occupation; (iii) essentially mean-field behavior for , where the MB effects are negligible even for . Thus both and at are enhanced by the increase of for , reduced for , and practically unaffected at . As functions of for a fixed , and have a maximum at and decrease monotonously with increasing , and do so more steeply the higher the . For and , and decrease monotonously with increasing , the decrease being quicker for higher and slower for higher . For , both
Keywords
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