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Hartree-Fock Approximation to the Heisenberg Antiferromagnet

Chi C. Sung

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Abstract

The properties of a Heisenberg antiferromagnet at low temperatures are calculated by assuming the two-sublattice structure and by using the double-time Green's-function formalism. The two-particle Green's function is decoupled according to the Hartree-Fock approximation, which differs from the random-phase approximation by an additional term. Since the two-particle Green's function in our problem contains particles of different lattices, the kinematical condition does not enter into this approximation. Numerical results for the ground-state energy and the magnetization are presented.

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The properties of a Heisenberg antiferromagnet at low temperatures are calculated by assuming the two-sublattice structure and by using the double-time Green's-function formalism. The two-particle Green's function is decoupled according to the Hartree-Fock approximation, which differs from the random-phase approximation by an additional term. Since the two-particle Green's function in our problem contains particles of different lattices, the kinematical condition does not enter into this approximation. Numerical results for the ground-state energy and the magnetization are presented.

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Available abstract

The properties of a Heisenberg antiferromagnet at low temperatures are calculated by assuming the two-sublattice structure and by using the double-time Green's-function formalism. The two-particle Green's function is decoupled according to the Hartree-Fock approximation, which differs from the random-phase approximation by an additional term. Since the two-particle Green's function in our problem contains particles of different lattices, the kinematical condition does not enter into this approximation. Numerical results for the ground-state energy and the magnetization are presented.

Key concepts: Random phase approximation, Physics, Born–Huang approximation, Ground state, Formalism (music), Hartree–Fock method, Quantum mechanics, Antiferromagnetism

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