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1
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0000857055
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M. Imada, A. Fujimori, and Y. Tokura: Rev. Mod. Phys. 70 (1998) 1039, and references therein.
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M. Imada, A. Fujimori, and Y. Tokura: Rev. Mod. Phys. 70 (1998) 1039, and references therein.
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2
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0001281275
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E. Dagotto, A. Moreo, F. Ortolani, D. Poilblanc, and J. Riera: Phys. Rev. B 45 (1992) 10741.
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(1992)
Phys. Rev. B
, vol.45
, pp. 10741
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Dagotto, E.1
Moreo, A.2
Ortolani, F.3
Poilblanc, D.4
Riera, J.5
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5
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33947238642
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The largest dimension of the subspace of the Hubbard model with a given Ns is realized at half filling with the same number of up-spin electrons and down-spin ones. For examples, the dimensions are 165 636 900 for Ns, 16, 2 363 904 400 for Ns, 18, and 34 134 779 536 for Ns, 20. It is possible to reduce these dimensions by using the symmetries of the Hamiltonian; however, the program for the reduced case is not necessarily applicable to any Hamiltonians having arbitrary shapes of clusters in contrast to our program. The versatile feature of our code makes it possible to examine the various cases very easily. Although the dimension is very huge, our code costs 29.7 h for the 260-time iterations to obtain the ground-state energy of the 20-site half-filling Hamiltonian for U, 35, when we use 16 nodes in the supercomputer SR11000 in Hokkaido University
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s = 20. It is possible to reduce these dimensions by using the symmetries of the Hamiltonian; however, the program for the reduced case is not necessarily applicable to any Hamiltonians having arbitrary shapes of clusters in contrast to our program. The versatile feature of our code makes it possible to examine the various cases very easily. Although the dimension is very huge, our code costs 29.7 h for the 260-time iterations to obtain the ground-state energy of the 20-site half-filling Hamiltonian for U = 35, when we use 16 nodes in the supercomputer SR11000 in Hokkaido University.
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12
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33947224935
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s = 18. These works use only the periodic boundary condition. Note that such behavior occurs only at the hole concentration when the electronic shell structure is open.
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s = 18. These works use only the periodic boundary condition. Note that such behavior occurs only at the hole concentration when the electronic shell structure is open.
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21
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0000330687
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S. Uchida, T. Ido, H. Takagi, T. Arima, Y. Tokura, and S. Tajima: Phys. Rev. B 43 (1991) 7942.
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(1991)
Phys. Rev. B
, vol.43
, pp. 7942
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Uchida, S.1
Ido, T.2
Takagi, H.3
Arima, T.4
Tokura, Y.5
Tajima, S.6
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