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(a) Goto, K.; Kubo, T.; Yamamoto, K.; Nakasuji, K.; Sato, K.; Shiomi, D.; Takui, T.; Kubota, M.; Kobayashi, T.; Takusi, K.; Ouyang, J. J. Am. Chem. Soc. 1999, 121, 1619.
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Prentice Hall: Englewood Cliffs, NJ
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(b) Williams, J. M.; Ferraro, J. R.; Thorn, R. J.; Carlson, K. D.; Geiser, U.; Wang, H. H.; Kini, A. M.; Whangbo, M.-H. Organic Superconductors (Including Fullerenes): Synthesis, Structure, Properties, and Theory; Prentice Hall: Englewood Cliffs, NJ, 1992.
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(b) Böhlin, J.; Hansson, A.; Stafström, S. Phys. Rev. B: Condens. Matter Mater. Phys. 2006, 74, 155111.
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27144481377
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Kubo, T.; Shimizu, A.; Sakamoto, M.; Uruichi, M.; Yakushi, K.; Nakano, M.; Shiomi, D.; Sato, K.; Takui, T.; Morita, Y.; Nakasuji, K. Angew. Chem., Int. Ed. 2005, 44, 6564. The crystal structure of 4 can be obtained from CCDC (deposition number 275077).
-
Kubo, T.; Shimizu, A.; Sakamoto, M.; Uruichi, M.; Yakushi, K.; Nakano, M.; Shiomi, D.; Sato, K.; Takui, T.; Morita, Y.; Nakasuji, K. Angew. Chem., Int. Ed. 2005, 44, 6564. The crystal structure of 4 can be obtained from CCDC (deposition number 275077).
-
-
-
-
30
-
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0032507270
-
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Ohashi, K.; Kubo, T.; Masui, T.; Yamamoto, K.; Nakasuji, K.; Takui, T.; Kai, Y.; Murata, I. J. Am. Chem. Soc. 1998, 120, 2018.
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Murata, I.8
-
32
-
-
33846985432
-
-
The bulky tert-butyl groups in 3 do not allow a face-to-face π-π intermolecular packing of the phenalenyl units, while this is possible for 1. This is because the tert-butyl groups of 3 are attached to spin-bearing C atoms and they bump into each other when forming π-stacking, while the tett-butyl groups of the π-dimer of 1 are staggered. In the case of 2, such a π-π intermolecular packing of the phenalenyl units is possible.
-
The bulky tert-butyl groups in 3 do not allow a face-to-face π-π intermolecular packing of the phenalenyl units, while this is possible for 1. This is because the tert-butyl groups of 3 are attached to spin-bearing C atoms and they bump into each other when forming π-stacking, while the tett-butyl groups of the π-dimer of 1 are staggered. In the case of 2, such a π-π intermolecular packing of the phenalenyl units is possible.
-
-
-
-
33
-
-
33846971790
-
-
Transfer integral t is used interchangeably with resonance integral β.
-
Transfer integral t is used interchangeably with resonance integral β.
-
-
-
-
34
-
-
33846980616
-
-
The term alternating chain does not mean the two resonance structures shown in Scheme 4 of ref 13, but means that the intermolecular and intramolecular interactions exist simultaneously, leading to two magnetic exchange parameters not equal to each other.
-
The term "alternating chain" does not mean the two resonance structures shown in Scheme 4 of ref 13, but means that the intermolecular and intramolecular interactions exist simultaneously, leading to two magnetic exchange parameters not equal to each other.
-
-
-
-
35
-
-
0004236045
-
-
See, for example:, VCH Publishers: New York
-
See, for example: Kahn, O. Molecular Magnetism; VCH Publishers: New York, 1993; pp 103-111.
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(1993)
Molecular Magnetism
, pp. 103-111
-
-
Kahn, O.1
-
36
-
-
33846959621
-
-
It is not a priori known which of the two exchange parameters corresponds to intra- and intermolecular interactions, respectively. The assignment of J1 to intramolecular and J2 to intermolecular interactions is based on transfer integrals associated with the intramolecular and intermolecular SOMO-SOMO overlaps. See the magnetism section
-
2 to intermolecular interactions is based on transfer integrals associated with the intramolecular and intermolecular SOMO-SOMO overlaps. See the magnetism section.
-
-
-
-
37
-
-
33846996536
-
-
Itoh, K, Kinoshita, M, Eds, Kodansha Ltd, Gordon and Beach Science Publishers: Tokyo, Amsterdam
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Kawakami, T. In Molecular Magnetism-New Magnetic Materials; Itoh, K., Kinoshita, M., Eds.; Kodansha Ltd., Gordon and Beach Science Publishers: Tokyo, Amsterdam, 2000: pp 9-10.
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, pp. 9-10
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Kawakami, T.1
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41
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33846988421
-
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Abecassis de Laredo, E, Jurisic, N. K, Eds, D. Reidel Publishing Co, Dordrecht-Holland, The Netherlands
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(c) Pincus, P. In Selected Topics in Physics, Astrophysics, and Biophysics; Abecassis de Laredo, E., Jurisic, N. K., Eds.; D. Reidel Publishing Co.: Dordrecht-Holland, The Netherlands, 1973; p 152.
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(1973)
Selected Topics in Physics, Astrophysics, and Biophysics
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Pincus, P.1
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42
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33846946973
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Miller, J. S, Ed, Plenum Press: New York
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(d) Soos, Z. G.; Bondeson, S. R. In Extended Linear Chain Compounds; Miller, J. S., Ed.; Plenum Press: New York, 1983; Vol. 3, p 196.
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Extended Linear Chain Compounds
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-
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Soos, Z.G.1
Bondeson, S.R.2
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43
-
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33748211136
-
-
Short-range electron correlation plays a significant role in determining the U value. See Ohno, K.; Noguchi, Y.; Yokoi, T.; Ishii, S.; Takeda, J.; Furuya, M. ChemPhysChem 2006, 7, 1820. The larger the SOMO electron delocalization domain, the smaller the U value because the two electrons have larger space to avoid each other.
-
(a) Short-range electron correlation plays a significant role in determining the U value. See Ohno, K.; Noguchi, Y.; Yokoi, T.; Ishii, S.; Takeda, J.; Furuya, M. ChemPhysChem 2006, 7, 1820. The larger the SOMO electron delocalization domain, the smaller the U value because the two electrons have larger space to avoid each other.
-
-
-
-
44
-
-
33846957533
-
-
For an example of U = ca. 1 eV for organic radicals with intermediate domains, see, for example: Tanner, D. B. In Extended Linear Chain Compounds; Miller, J. S., Ed.; Plenum Press: New York, 1983; 2, p 205.
-
(b) For an example of U = ca. 1 eV for organic radicals with intermediate domains, see, for example: Tanner, D. B. In Extended Linear Chain Compounds; Miller, J. S., Ed.; Plenum Press: New York, 1983; Vol. 2, p 205.
-
-
-
-
45
-
-
33846969727
-
-
For the U value of ca. 1 eV for the title compounds, see refs. 13 and 14.
-
(c) For the U value of ca. 1 eV for the title compounds, see refs. 13 and 14.
-
-
-
-
47
-
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33846968632
-
-
Frisch, M. J.; et al. Gaussian 03, revision B.04; Gaussian, Inc.: Pittsburgh, PA, 2003.
-
Frisch, M. J.; et al. Gaussian 03, revision B.04; Gaussian, Inc.: Pittsburgh, PA, 2003.
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49
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0345491105
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(b) Lee, C.; Yang, W.; Parr, R. G. Phys. Rev. B: Condens. Matter Mater. Phys. 1988, 37, 785.
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Lee, C.1
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53
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20544463457
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Using Vanderbilt-type (Vanderbilt, D. Phys. Rev. B: Condens. Matter Mater. Phys. 1990, 41, 7892) untrasoft pseudo-potentials
-
(c) Using Vanderbilt-type (Vanderbilt, D. Phys. Rev. B: Condens. Matter Mater. Phys. 1990, 41, 7892) untrasoft pseudo-potentials
-
-
-
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57
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0344588866
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(b) Ito, A.; Ino, H.; Ichiki, H.; Tanaka, K. J. Phys. Chem. A 2002, 106, 8716.
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Nixdorf, M.6
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62
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27744566839
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See in
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See in Kertesz, M.; Choi, C. H.; Yang, S. Chem. Rev. 2005, 105, 3448.
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Kertesz, M.1
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66
-
-
33846952990
-
-
This may result from the substitution of tert-butyl groups since in the case of 2 all bond distances agree with those of the unsubstituted BPBR including bonds f and i see Table 2
-
This may result from the substitution of tert-butyl groups since in the case of 2 all bond distances agree with those of the unsubstituted BPBR including bonds f and i (see Table 2).
-
-
-
-
68
-
-
0042874331
-
-
Watson, W. H.; Kashyap, R. P.; Plummer, B. F.; Reese, W. G. Acta Crystallog., Sect. C: Cryst. Struct. Commun. 1991, 47, 1848.
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Acta Crystallog., Sect. C: Cryst. Struct. Commun
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Watson, W.H.1
Kashyap, R.P.2
Plummer, B.F.3
Reese, W.G.4
-
69
-
-
33846966116
-
-
Fully optimized bond distances of a through k for complex 5 are (in Å): 1.468, 1.444, 1.404, 1.397, 1.414, 1.428, 1.396, 1.407, 1.426, 1.395, and 1.416.
-
Fully optimized bond distances of a through k for complex 5 are (in Å): 1.468, 1.444, 1.404, 1.397, 1.414, 1.428, 1.396, 1.407, 1.426, 1.395, and 1.416.
-
-
-
-
70
-
-
0018467666
-
-
See for example
-
See for example: Whangbo, M.-H.; Hoffmann, R.; Woodward, R. B. Proc. R. Soc. London, Ser. A 1979, 366, 23.
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Proc. R. Soc. London, Ser. A
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-
-
Whangbo, M.-H.1
Hoffmann, R.2
Woodward, R.B.3
-
71
-
-
33846968631
-
-
2 = 0.9914.
-
2 = 0.9914.
-
-
-
-
72
-
-
33846954903
-
-
2 = 0.46 eV.
-
2 = 0.46 eV.
-
-
-
-
73
-
-
0344236180
-
-
(a) Senthikumar, K.; Grozema, F. C.; Bickelhaupt, F. M.; Siebbeles, L. D. A. J. Chem. Phys. 2003, 119, 9809.
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Senthikumar, K.1
Grozema, F.C.2
Bickelhaupt, F.M.3
Siebbeles, L.D.A.4
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74
-
-
0037197928
-
-
(b) Brédas, J. L.; Calbert, J. P.; da Silva Filho, D. A.; Cornil, J.; Proc. Natl. Acad. Sci. U.S.A. 2002, 99, 5804.
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Proc. Natl. Acad. Sci. U.S.A
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Brédas, J.L.1
Calbert, J.P.2
da Silva Filho, D.A.3
Cornil, J.4
-
75
-
-
33847000717
-
-
P is on a per mol of BPBR molecule basis with two spins for each molecule.
-
P is on a per mol of BPBR molecule basis with two spins for each molecule.
-
-
-
-
76
-
-
27544441189
-
-
For using Curie-Weiss law for impurities, see for example
-
(a) For using Curie-Weiss law for impurities, see for example: Belik, A. A.; Azuma, M.; Takano, M. Inorg. Chem. 2005, 44, 7523.
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(2005)
Inorg. Chem
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-
-
Belik, A.A.1
Azuma, M.2
Takano, M.3
-
77
-
-
33846975952
-
-
Curie law can be used instead, where θ is approximated to be 0 if the residual χ(T)T coming from the paramagnetic impurity remains constant at low temperature.
-
(b) Curie law can be used instead, where θ is approximated to be 0 if the residual χ(T)T coming from the paramagnetic impurity remains constant at low temperature.
-
-
-
-
79
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