Spin-Waves in Stoner Ferromagnetic Phase of a Two-Dimensional Electron System
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We have studied the collective excitations (spin-wave energies) in the ground state of a two-dimensional (2D) electron system using the random phase approximation (RPA). To do so, we have calculated the magnetic transverse susceptibility in 2D electron system by Hartree-Fock (HF) approximation of Hubbard model at T=0 which is generally referred to as the Stoner model. The spin-waves dispersion of three-dimensional (3D) electron system due to its quadratic behavior starts from zero at q0 while our numerical results show that the spin-waves dispersion of 2D electron system starts from the value Δ, known as exchange splitting energy, even at q=0.
THE POLARON EFFECTS AND RELAXATION OF NON-EQUILIBRIUM ELECTRONS IN THE QUASI-TWO-DIMENSIONAL SYSTEMS
1991 ◽
Vol 05
(02)
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pp. 139-149
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2002 ◽
Vol 57
(2-3)
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pp. 11
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1975 ◽
Vol 39
(2)
◽
pp. 279-288
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