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25
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33744558875
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note
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Depending an the strength of the interelectron repulsion, WM's can also form at zero magnetic field; see Refs. 13, 20, and 21. For a CPD/exact-solution study of such WM's at B = 0, see Ref. 24.
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28
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4243943579
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A certain degree of Wigner crystallization has also been found in another geometry, i.e., in an infinite Hall bar at an integral filling factor v = 2; see J.P. Rodriguez, M.J. Franco, and L. Brey, Phys. Rev. B 61, 16787 (2000).
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Rodriguez, J.P.1
Franco, M.J.2
Brey, L.3
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30
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33744705854
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note
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In our earlier publications (Refs. 13, 14, 20, and 21), we have used the term spin-and-space (sS)-UHF to emphasize the breaking of both the spin and space symmetries. In this paper, only the breaking of the space symmetry is involved.
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31
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33744670953
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note
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L operator used for restoring the circular symmetry in the simplest (0,N) and (1,N-1) ring arrangements (Ref. 21), or for objects without a ring structure (Ref. 19).
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-
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33
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33744658731
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note
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The magic angular momenta for N≤7 have been also discussed in the context of the geometric configuration (Refs. 9 and 10) and the Eckart frame (Ref. 11) models. However, unlike our approach, these models do not afford derivation of analytical forms for the REM wave functions.
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34
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33744580212
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note
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The REM functions also have close-to-unity overlaps with the exact wave functions. For an example, see Table II in ArXiv: cond-mat/0202062 (unpublished).
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35
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33744688651
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note
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3=7.
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