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1
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35348880477
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For recent reviews see, Chem. Rev. 104 (2004) No. 11, Issue on Molecular Conductors;
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For recent reviews see, Chem. Rev. 104 (2004) No. 11, Issue on Molecular Conductors;
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2
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35348835586
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J. Phys. Soc. Jpn. 75 (2006) No. 5, Special Topics section on Organic Conductors.
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J. Phys. Soc. Jpn. 75 (2006) No. 5, Special Topics section on Organic Conductors.
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4
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0034250645
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D. S. Chow, F. Zamborszky, B. Alavi, D. J. Tantillo, A. Baur, C. A. Merlic, and S. E. Brown: Phys. Rev. Lett. 85 (2000) 1698.
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Phys. Rev. Lett
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Chow, D.S.1
Zamborszky, F.2
Alavi, B.3
Tantillo, D.J.4
Baur, A.5
Merlic, C.A.6
Brown, S.E.7
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9
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0037104302
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F. Zamborszky, W. Yu, W. Raas, S. E. Brown, B. Alavi, C. A. Merlic, and A. Baur: Phys. Rev. B 66 (2002) 081103.
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(2002)
Phys. Rev. B
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Zamborszky, F.1
Yu, W.2
Raas, W.3
Brown, S.E.4
Alavi, B.5
Merlic, C.A.6
Baur, A.7
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10
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10344252147
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W. Yu, F. Zhang, F. Zamborszky, B. Alavi, A. Baur, C. A. Merlic, and S. E. Brown: Phys. Rev. B 70 (2004) 121101.
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(2004)
Phys. Rev. B
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Yu, W.1
Zhang, F.2
Zamborszky, F.3
Alavi, B.4
Baur, A.5
Merlic, C.A.6
Brown, S.E.7
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11
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33846875236
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T. Kakiuchi, Y. Wakabayashi, H. Sawa, T. Itou, and K. Kanoda: Phys. Rev. Lett. 98 (2007) 066402.
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(2007)
Phys. Rev. Lett
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Kakiuchi, T.1
Wakabayashi, Y.2
Sawa, H.3
Itou, T.4
Kanoda, K.5
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15
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18844454745
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S. Ejima, F. Gebhard, and S. Nishimoto: Europhys. Lett. 70 (2005) 492, and references therein.
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S. Ejima, F. Gebhard, and S. Nishimoto: Europhys. Lett. 70 (2005) 492, and references therein.
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17
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33845534579
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S. Ejima, F. Gebhard, and S. Nishimoto: Phys. Rev. B 74 (2006) 245110, and references therein.
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S. Ejima, F. Gebhard, and S. Nishimoto: Phys. Rev. B 74 (2006) 245110, and references therein.
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18
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35348896760
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In the presence of alternation in transfer integrals, the CO state may be called a co-existence of the dimer-Mott insulator and CO since dimerization is always present; in this paper we call this simply as the CO state
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In the presence of alternation in transfer integrals, the CO state may be called a co-existence of the dimer-Mott insulator and CO since dimerization is always present; in this paper we call this simply as the CO state.
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24
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33847265471
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H. Seo, K. Tsutsui, M. Ogata, and J. Merino: J. Phys. Soc. Jpn. 75 (2006) 114707, and references therein.
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H. Seo, K. Tsutsui, M. Ogata, and J. Merino: J. Phys. Soc. Jpn. 75 (2006) 114707, and references therein.
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25
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35348814499
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We do not consider the 2kF-CDW state with a 4-fold periodicity along the chains since we are interested in stability of Wigner crystal-type charge ordering
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F-CDW state with a 4-fold periodicity along the chains since we are interested in stability of Wigner crystal-type charge ordering.
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28
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84858355262
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ρ in eq. (4), should be multiplied by -1/2 in order to reproduce the Hamiltonian in ref. 16. The change in the sign is due to the choice of the Klein factor.
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ρ in eq. (4), should be multiplied by -1/2 in order to reproduce the Hamiltonian in ref. 16. The change in the sign is due to the choice of the Klein factor.
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