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T. J. Emge, H. H. Wang, P. C. W. Leung, P. R. Rust, J. D. Cook, P. L. Jackson, K. D. Carlson, J. M. Williams, M.-H. Whangbo, E. L. Venturini, J. E. Shirber, L. J. Azevedo and J. R. Ferraro, J. Am. Chem. Soc., 1986, 108, 695.
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4
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0037138601
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x, for one particular composition (x = 0.66) upon doping by a mono-anion; see: H. Mori, M. Masakazu, M. Haemori, H. Suzuki, S. Tanaka, Y. Nisio, K. Kajita and H. Motiyama, J. Am. Chem. Soc., 2002, 124, 1251.
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0001680508
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0942286650
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note
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(b) note that although there can be small differences in details the βHOMO-HOMO interaction energies and the associated transfer integrals (t) are obviously related and have the same physical meaning. However, because overlap is explicitly taken into account in extended Hückel calculations, the absolute values of β are somewhat larger than those of t. We use the β values here because it facilitates the comparison with other calculations for β ′ salts already reported in the literature.
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10
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0037885010
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2 becomes a superconductor at 14.2 K under high hydrostatic pressure (8.2 GPa); see: H. Taniguchi, M. Miyashita, K. Uchiyama, K. Satoh, N. Mori, H. Okamoto, K. Miyagawa, K. Kanoda, M. Hedo and Y. Uwatoko, J. Phys. Soc. Jpn., 2003, 72, 468.
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Okamoto, H.6
Miyagawa, K.7
Kanoda, K.8
Hedo, M.9
Uwatoko, Y.10
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33947092746
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(b) J. Ammeter, H.-B. Bürgi, J. Thibeault and R. Hoffmann, J. Am. Chem. Soc., 1978, 100, 3686.
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Ammeter, J.1
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Hoffmann, R.4
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