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CIORGA M., SACHRAJDA A. S., HAWRYLAK P., GOULD C., ZAWADZKI P., JULLIAN S., FENG Y. and WASILEWSKI Z., Phys. Rev. B, 61 (2000) R16315.
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Jullian, S.6
Feng, Y.7
Wasilewski, Z.8
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8
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0033618617
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ZHITENEV N. B., BRODSKY M., ASHOORI R. C., PFEIFFER L. N. and WEST K. W., Science, 285 (1999) 715.
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Zhitenev, N.B.1
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9
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0031235080
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ZHITENEV N. B., ASHOORI R. C., PFEIFFER L. N. and WEST K. W., Phys. Rev. Lett., 79 (1997) 2308.
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10
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4243385961
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s a second stage of Wigner crystallization has been discussed by FILINOV A. V., BONITZ M. and LOZOVIK YU. E., Phys. Rev. Lett., 86 (2001) 3851, where the inter-shell rotation is suppressed. However, this phenomenon is not further discussed here.
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Filinov, A.V.1
Bonitz, M.2
Lozovik, Yu.E.3
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16
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0141780232
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note
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Experimentally observable addition energies are determined by free energy differences. However, at the low temperature considered here, entropic contributions are very small. This has been checked for several N.
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21
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0141556942
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Further improvement is possible using the multi-level blocking approach [6] to alleviate the sign problem. However, it was not used here to allow for arbitrary Δτ
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Further improvement is possible using the multi-level blocking approach [6] to alleviate the sign problem. However, it was not used here to allow for arbitrary Δτ.
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25
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0037084702
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MATAGNE P., LEBURTON J. P., AUSTING D. G. and TARUCHA S., Phys. Rev. B, 65 (2002) 085325.
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Matagne, P.1
Leburton, J.P.2
Austing, D.G.3
Tarucha, S.4
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26
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0141668308
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For N = 9, 10, the ground-state spins were derived from finite-Δτ data not given in table I
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For N = 9, 10, the ground-state spins were derived from finite-Δτ data not given in table I.
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28
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0032179744
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ASHOORI R. C., ZHITENEV N. B., PFEIFFER L. and WEST K., Physica E, 3 (1998) 15.
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(1998)
Physica E
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Ashoori, R.C.1
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Pfeiffer, L.3
West, K.4
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