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I. Affleck: Nucl. Phys. B 336 (1996) 517; I. Affleck and A. W. W. Ludwig: Nucl. Phys. B 360 (1991) 641; Phys. Rev. Lett. 67 (1991) 3160; S. Eggert and I. Affleck: Phys. Rev. B 46 (1992) 10866; P. Fröjdh and H. Johannesson: ibid. 53 (1996) 3211.
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I. Affleck: Nucl. Phys. B 336 (1996) 517; I. Affleck and A. W. W. Ludwig: Nucl. Phys. B 360 (1991) 641; Phys. Rev. Lett. 67 (1991) 3160; S. Eggert and I. Affleck: Phys. Rev. B 46 (1992) 10866; P. Fröjdh and H. Johannesson: ibid. 53 (1996) 3211.
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Phys. Rev. B
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Eggert, S.1
Affleck, I.2
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5
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0040924383
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I. Affleck: Nucl. Phys. B 336 (1996) 517; I. Affleck and A. W. W. Ludwig: Nucl. Phys. B 360 (1991) 641; Phys. Rev. Lett. 67 (1991) 3160; S. Eggert and I. Affleck: Phys. Rev. B 46 (1992) 10866; P. Fröjdh and H. Johannesson: ibid. 53 (1996) 3211.
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Fröjdh, P.1
Johannesson, H.2
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Phys. Rev. B
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13
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85033154753
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note
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The final results are found to be insensitive to the choices unless extreme distributions are assumed.
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14
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85033140675
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note
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As discussed in ref. 5, there must be an upper limit to the system size for high temperatures, since the number of discarded states increases with increasing system size.
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15
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0003517424
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ed. M. Suzuki Springer-Verlag, Berlin
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See, for example, M. Takasu, S. Miyashita and M. Suzuki: Quantum Monte Carlo Methods, ed. M. Suzuki (Springer-Verlag, Berlin, 1987) p. 114.
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Quantum Monte Carlo Methods
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Takasu, M.1
Miyashita, S.2
Suzuki, M.3
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