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1
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85037889679
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Gordon Baym, Lectures on Quantum Mechanics (Benjamin/Cummings, Reading, MA, 1969), pp. 148–168.
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Gordon Baym, Lectures on Quantum Mechanics (Benjamin/Cummings, Reading, MA, 1969), pp. 148–168.
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2
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85037873102
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Claude Itzykson and Jean-Bernard Zuber, Quantum Field Theory (McGraw-Hill, New York, 1980), pp. 513–519.
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Claude Itzykson and Jean-Bernard Zuber, Quantum Field Theory (McGraw-Hill, New York, 1980), pp. 513–519.
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9
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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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Kouwenhoven, L.P.1
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Eto, M.4
Austing, D.G.5
Honda, T.6
Tarucha, S.7
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10
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0000715254
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The self-conjugate representation of SU(4) differs from the fundamental representation considered recently by Y. Yamashita, N. Shibata, and K. Ueda, Phys. Rev. B 58, 9114 (1998). There is one electron in the fundamental representation, which therefore has dimension 4 and corresponds to quarter filling. At half-filling there are the two electrons, and the representation is self-conjugate.
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Phys. Rev. B
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Yamashita, Y.1
Shibata, N.2
Ueda, K.3
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11
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0000818466
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A more precise calculation of the exchange constant (Formula presented) is presented in G. Burkard, D. Loss, and D. P. DiVincenzo, Phys. Rev. B 59, 2070 (1999).
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Phys. Rev. B
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Burkard, G.1
Loss, D.2
DiVincenzo, D.P.3
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12
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85037878907
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Spin-orbit splitting of the (Formula presented) states is (Formula presented) to (Formula presented) times smaller than (Formula presented) because the splitting is of order (Formula presented) where (Formula presented) is the fine-structure constant and (Formula presented) is the number of electrons in the dot [G. Baym, Lectures on Quantum Mechanics (Ref. 1), pp. 460–465].
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Spin-orbit splitting of the (Formula presented) states is (Formula presented) to (Formula presented) times smaller than (Formula presented) because the splitting is of order (Formula presented) where (Formula presented) is the fine-structure constant and (Formula presented) is the number of electrons in the dot [G. Baym, Lectures on Quantum Mechanics (Ref. 1), pp. 460–465].
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17
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0030521429
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M. Fricke, H. Lorke, J. P. Kotthaus, G. Medeiros-Ribeiro, and P. M. Petroff, Europhys. Lett. 36, 197 (1996).
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Petroff, P.M.5
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0029849866
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C. Livermore, C. H. Crouch, R. M. Westervelt, K. L. Campman, and A. C. Gossard, Science 274, 1332 (1996).
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21
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0000311307
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Perturbation in powers of (Formula presented) has been worked out for the SU(2) Hubbard model. See D. J. Klein and W. A. Seitz, Phys. Rev. B 8, 2236 (1973);
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0040778131
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I. Affleck, D. Arovas, J. B. Marston, and D. Rabson, Nucl. Phys. B 366, 467 (1991).
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27
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85037882772
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The double-precision, vectorized, multiprocessor (Formula presented) code for the DMRG is run on a Cray EL-98 and J-916 computers [A. V. Onufriev and J. B. Marston (unpublished)].
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The double-precision, vectorized, multiprocessor (Formula presented) code for the DMRG is run on a Cray EL-98 and J-916 computers [A. V. Onufriev and J. B. Marston (unpublished)].
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28
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85037896853
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The completely dimerized state is an exact ground state of (Formula presented) as may be shown by rewriting (Formula presented) as a sum of projection operators.
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The completely dimerized state is an exact ground state of (Formula presented) as may be shown by rewriting (Formula presented) as a sum of projection operators.
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30
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26844535199
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K. Leo, J. Shah, E. O. Gobel, T. C. Damen, S. Schmittrink, W. Schafer, and K. Kohler, Phys. Rev. Lett. 66, 201 (1991).
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See, for instance, D. P. DiVincenzo, Science 270, 255 (1995);
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D. Goldhaber-Gordon, H. Shtrikman, D. Mahalu, D. Abusch-Magder, U. Meirav, and M. A. Kastner, Nature (London) 391, 156 (1998);
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Kastner, M.A.6
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43
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85037913989
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See, for instance, Charles Kittel, Introduction to Solid State Physics (Wiley, New York, 1996).
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See, for instance, Charles Kittel, Introduction to Solid State Physics (Wiley, New York, 1996).
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