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Physics-Uspekhi

Ground states in one-dimensional electron systems

W. Hansen, D. Schmerek, Chr. Steinebach

Published Feb 28, 1998• 7 citations
Publisher
DOI
10.1070/pu1998v041n02abeh000357

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A theorem about the spin properties of the ground state and the ordering of the energy levels for different spins of an interacting-electron model including an arbitrary diagonal interacting potential, an antiferromagnetic exchange, and an electron pair-hopping term for particles on a one-dimensional lattice is stated and proved. We show that when the number of electrons N = 4n + 2 (n an integer) with periodic boundary conditions or N = 4n with antiperiodic boundary conditions, the ground state is a nondegenerate singlet. This theorem generalizes a similar theorem Lieb and Mattis proved for the one-dimensional interacting electron system.
We present an accurate diffusion Monte Carlo computation of the ground state of a two-dimensional electron gas laterally confined by a harmonic potential in the effective mass-dielectric constant approximation. The computation is made explicitly including the second dimension, and can therefore address the occurrence of phase transitions in the system. The system was studied as a function of the one-dimensional Wigner-Seitz parameter ${r}_{s}=1/2{\ensuremath{\rho}}^{1\text{D}}$ in the range $0.5\ensuremath{\le}{r}_{s}\ensuremath{\le}7$. The ground state is found to be spin polarized for rs>3{r}_{s}>3rs​>3.