摘要
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.
原文 | English |
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頁(從 - 到) | 395-398 |
頁數 | 4 |
期刊 | Physics Letters A |
卷 | 116 |
發行號 | 8 |
DOIs | |
出版狀態 | Published - 7 7月 1986 |