Abstract
The two-dimensional interacting electron gas under a strong homogeneous magnetic field is approximated by the one-dimensional classical lattice gas. We show that in our model the eigenstates of the system approach single-particle Slater determinants in the large particle number limit. Cusps in the energy of our model are found at simple fractional occupations.
Original language | English |
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Pages (from-to) | 395-398 |
Number of pages | 4 |
Journal | Physics Letters A |
Volume | 116 |
Issue number | 8 |
DOIs | |
State | Published - 7 Jul 1986 |