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33646669841
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note
-
The exchange energy J(B⊥,B∥) results from both single-particle and Coulomb contributions. The term exchange interaction, as used in the paper, indicates only the Coulomb term depending on the symmetry of the two-electron spatial wave function.
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25
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0034138835
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Y. Tokura, S. Sasaki, D.G. Austing, and S. Tarucha, Physica E (Amsterdam) 6, 676 (2000).
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33646665857
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note
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0 = 0.067, ε* = 12.9, g* = -0.44.
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-
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27
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33646660541
-
-
note
-
Typical calculations are performed on a (100×100×40) nm grid with (64×64×128) points along directions (x,y,z), respectively; the Coulomb interaction is represented on a single-particle basis set consisting of 12 states.
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-
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29
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33646664557
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note
-
Here the S/AS labeling is used for brevity. Obviously, for a general field direction with respect to the tunneling direction, wave functions do not have a well defined S/AS symmetry. See Bellucci et al. (Ref. 25).
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-
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30
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33646643217
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note
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g) molecular orbitals, respectively. See Rontani et al. (Ref. 7).
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-
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32
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33646669476
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note
-
Eventually, as the field is further increased, electron localize in a confined counterpart of a Wigner crystal. See Rontani et al. (Ref. 9).
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33
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0030667406
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L.P. Kouwenhoven, T.H. Oosterkamp, M.W.S. Danoesastro, M. Eto, D.G. Austing, T. Honda, and S. Tarucha, Science 278, 1788 (1997).
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1842633271
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D. Bellucci, M. Rontani, G. Goldoni, F. Troiani, and E. Molinari, Physica E (Amsterdam) 22, 482 (2004).
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35
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33646666265
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note
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Scattering of calculated points is related to the finiteness of the space grids. These inaccuracies are more significant for nonsymmetric field directions.
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