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  • Access by Xinjiang University

Theory of Inelastic Neutron Scattering in the Itinerant Model Antiferromagnetic Metals. I

J. B. Sokoloff

  • Brookhaven National Laboratory, Upton, New York 11973

Phys. Rev. 185, 770 – Published 10 September, 1969

DOI: https://doi.org/10.1103/PhysRev.185.770

Abstract

The susceptibility functions χ+(K, ω) and χzz(K, ω) are calculated in the random-phase approximation at zero temperature for the Slater model of itinerant antiferromagnetism using the Hubbard Hamiltonian; from these susceptibility functions the neutron-scattering cross section is calculated. A pole is found in χ+(K, ω) corresponding to a spin-wave model As in the Heisenberg model of spin waves, the residue of this pole approaches zero as the scattering vector K approaches a chemical reciprocal lattice vector τ, and becomes infinite as K approaches a magnetic reciprocal-lattice vector Q. The non-spin-flip single-particle-mode scattering is found to become infinite at an energy corresponding to the magnetic splitting of the bands at the boundary of the magnetic Brillouin zone if the Fermi level lies in this gap. If the Fermi level does not lie in the gap, then there is a pole in χzz(K, ω) for K near a magnetic reciprocal-lattice vector, at an energy equal to the gap energy when K = Q, corresponding to a collective excitation. Acoustic plasmon poles in χzz(q, ω) are also discussed.

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