From independent particle towards collective motion for two polarized electrons on a square lattice |
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Authors: | M Martínez J-L Pichard |
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Institution: | (1) CEA/DSM, Service de Physique de l'état Condensé, Centre d'études de Saclay, 91191, Gif-sur-Yvette Cedex, France, FR |
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Abstract: | The two dimensional crossover from independent particle towards collective motion is studied using 2 polarized electrons (spinless
fermions) interacting via a U/r Coulomb repulsion in a L×L square lattice with periodic boundary conditions and nearest neighbor hopping t. Three regimes characterize the ground state when U/t increases. Firstly, when the fluctuation Δr of the spacing r between the two particles is larger than the lattice spacing a, there is a scaling length L
0 = π2(t/U) such that the relative fluctuation Δr/〈r〉 is a universal function of the dimensionless ratio L/L
0, up to finite size corrections of order L-2. L < L
0 and L > L
0 are respectively the limits of the free particle Fermi motion and of the correlated motion of a Wigner molecule. Secondly,
when U/t exceeds a threshold U
*(L)/t, Δr becomes smaller than a, giving rise to a correlated lattice regime where the previous scaling breaks down and analytical expansions in powers of
t/U become valid. A weak random potential reduces the scaling length and favors the correlated motion.
Received 28 March 2002 Published online 19 November 2002 |
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Keywords: | PACS 71 10 -w Theories and models for many-electron systems – 71 27 +a Strongly correlated electron systems – 73 20 Qt Electron solids |
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