Hydrogen atoms were located at the calculated positions. The
final R and Rw values are 0.044 and 0.109 for 7473 reflections
with I > 2rI and 559 parameters. Estimated standard deviations
at the calculated positions. The final R and Rw values are 0.068
and 0.176 for 5013 reflections with I > 2rI and 532 parameters.
˚
Estimated standard deviations for rac-9c are 0.003–0.005 A for
◦
bond lengths and 0.2–0.3◦ for bond angles.
˚
are 0.002–0.003 A for bond lengths and 0.1–0.2 for bond angles.
Crystal data for rac-5c. C48H30O2, M 638.76, yellow needle,
0.1 × 0.03 × 0.03 mm, monoclinic P21/n, a = 11.977(3), b =
References
3
˚
˚
24.465(6), c = 12.250(4) A, b = 110.328(2), V = 3365.8(1) A ,
q(Z = 4) = 1.260 g cm−1. A total of 7457 unique data (2hmax
=
1 (a) R. Mayer and K. Kro¨ber, J. Prakt. Chem., 1974, 316, 907; (b) U.
Scho¨berl, J. Salbeck and J. Daub, Adv. Mater., 1992, 4, 41; (c) D.
Lorcy, R. Carlier, A. Robert, A. Tallec, P. Le Maguere`s and L.
Ouahab, J. Org. Chem., 1995, 60, 2443; (d) P. Hapiot, D. Lorcy, A.
Tallec, R. Carlier and A. Robert, J. Phys. Chem., 1996, 100, 14823;
(e) A. Benahmed-Gasmi, P. Fre`re, J. Roncali, E. Elandaloussi, J.
Ordun, J. Garin, M. Jubault and A. Gorgues, Tetrahedron Lett.,
1995, 36, 2983; (f) A. J. Moore, M. R. Bryce, P. J. Skabara, A. S.
Batsanov, L. M. Goldenberg and J. A. K. Howard, J. Chem. Soc.,
Perkin Trans. 1, 1997, 3443; (g) P. Hascoat, D. Lorcy, A. Robert,
R. Carlier, A. Tallec, K Boubekeur and P. Batail, J. Org. Chem.,
1997, 62, 6086; (h) A. Ohta and Y. Yamashita, J. Chem. Soc., Chem.
Commun., 1995, 1761; (i) Y. Yamashita, M. Tomura, M. B. Zaman
and K. Imaeda, Chem. Commun., 1998, 1657.
2 (a) S. Hu¨nig, M. Kemmer, H. Wenner, F. Barbosa, G. Gescheidt, I. F.
Perepichka, P. Ba¨uerle, A. Emge and K. Peters, Chem. Eur. J., 2000,
6, 2618; (b) S. Hu¨nig, M. Kemmer, H. Wenner, I. F. Perepichka, P.
Ba¨uerle, A. Emge and G. Gescheid, Chem. Eur. J., 1999, 5, 1969.
3 (a) J. C. Traeger, J. Phys. Chem., 1986, 90, 4114; (b) G. Renzi, A.
Lombardozzi, E. Dezi, A. Pizzabiocca and M. Speranza, Chem.
Eur. J., 1996, 2, 316.
4 (a) T. Suzuki, H. Higuchi, M. Ohkita and T. Tsuji, Chem. Commun.,
2001, 1574; (b) H. Higuchi, E. Ohta, H. Kawai, K. Fujiwara, T.
Tsuji and T. Suzuki, J. Org. Chem., 2003, 68, 6605; (c) T. Suzuki, S.
Tanaka, H. Higuchi, H. Kawai and K. Fujiwara, Tetrahedron Lett.,
2004, 45, 8563; (d) H. Kawai, T. Takeda, K. Fujiwara and T. Suzuki,
Tetrahedron Lett., 2004, 45, 8289.
5 P. M. S. Monk, R. J. Mortimer and D. R. Rosseinsky, Elec-
trochromism: Fundamentals and Applications, VHC, Weinheim, 1995.
6 T. Suzuki, H. Higuchi, T. Tsuji, J. Nishida, Y. Yamashita and T.
Miyashi, Chemistry of Nanomolecular Systems. Chapter 1: Dynamic
Redox Systems, T. Nakamura, T. Matsumoto, T. Tada and K. Sug-
iura, eds; Springer, Hidelberg, 2003, pp. 3–24.
7 S. Iwashita, E. Ohta, H. Higuchi, H. Kawai, K. Fujiwara, K. Ono,
M. Takenaka and T. Suzuki, Chem. Commun., 2004, 2076.
8 (a) N. C. Deno, J. J. Jaruzelski and A. Schriesheim, J. Am. Chem.
Soc., 1955, 77, 3044; (b) R. J. Goldacre and J. N. Phillips, J. Chem.
Soc., 1949, 1724; (c) E. M. Arnett, R. A. Flowers, II, R. T. Ludwig,
A. E. Meekhof and S. A Walek, J. Phys. Org. Chem., 1997, 10, 499.
9 L. Pauling, The Nature of Chemical Bond and the Structure of
Molecules and Crystals, 3rd edn., Cornell University Press, Ithaca,
NY, 1960.
10 N. Berova, K. Nakanishi and R. W. Woody, Circular Dichroism:
Principles, Applications, 2nd edn., Wiley-VCH, New York, 2000.
11 (a) P. R. Markies, A. Villena, O. S. Akkerman, F. Bickelhaupt, W. J. J.
Smeets and A. L. Spek, J. Organomet. Chem., 1993, 463, 7; (b) C. C.
Barker and G. Hallas, J. Chem. Soc., 1961, 2642; (c) H. Kawai, T.
Nagasu, T. Takeda, K. Fujiwara, T. Tsuji, M. Ohkita, J. Nishida and
T. Suzuki, Tetrahedron Lett., 2004, 45, 4553.
55◦) were measured at T = 293 K by a Rigaku Mercury
˚
CCD apparatus (Mo-Ka radiation, k = 0.71069 A, 50 kV,
200 mA). Absorption correction was applied (l = 0.75 cm−1).
The structure was solved by the direct method (SIR92) and
refined by the full-matrix least-squares method on F2 (all data)
with anisotropic temperature factors for non-hydrogen atoms.
Hydrogen atoms were located at the calculated positions. The
final R and Rw values are 0.062 and 0.164 for 2329 reflections
with I > 2rI and 451 parameters. Estimated standard deviations
◦
˚
are 0.005–0.01 A for bond lengths and 0.4–0.7 for bond angles.
Crystal data for rac-6b2+(SbCl6−)2. C52H42Cl12O4Sb2, M
1399.84, red platelet, 0.2 × 0.2 × 0.05 mm, monoclinic C2/m,
˚
a = 18.425(7), b = 34.50(1), c = 10.674(4) A, b = 115.457(3),
3
−1
˚
V = 6125.4(3) A , q(Z = 4) = 1.518 g cm . A total of 7050
unique data (2hmax = 55◦) were measured at T = 293 K by
a Rigaku Mercury CCD apparatus (Mo-Ka radiation, k =
˚
0.71069 A, 50 kV, 200 mA). Absorption correction was applied
(l = 14.43 cm−1). The structure was solved by the direct method
(SIR92) and refined by the full-matrix least-squares method on
F2 (all data) with the anisotropic temperature factors for non-
hydrogen atoms. Hydrogen atoms were located at the calculated
positions. The final R and Rw values are 0.054 and 0.160 for
1874 reflections with I > 2rI and 322 parameters. Estimated
standard deviations for 6b2+ are 0.008–0.010 A for bond lengths
˚
and 0.4–0.9◦.
−
Crystal data for rac-6c2+(SbCl6
) dichloromethane solvate.
2
C50.5H30Cl15O2Sb2, M 1444.09, black platelet, 0.2 × 0.05 ×
0.01 mm, orthorhombic Fdd2, a = 57.17(1), b = 35.880(9), c =
3
−1
˚
˚
10.483(3) A, V = 21504(8) A , q(Z = 16) = 1.789 g cm . A total
of 6324 unique data (2hmax = 55◦) were measured at T = 153 K
by a Rigaku Mercury CCD apparatus (Mo-Ka radiation, k =
˚
0.71069 A, 50 kV, 200 mA). Absorption correction was applied
(l = 17.89 cm−1). The structure was solved by the direct method
(SIR92) and refined by the full-matrix least-squares method on
F2 (all data) with the anisotropic temperature factors for non-
hydrogen atoms. Hydrogen atoms were located at the calculated
positions. The final R and Rw values are 0.056 and 0.2134 for
1582 reflections with I > 2rI and 611 parameters. Estimated
standard deviations for 6c2+ are 0.02–0.03 A for bond lengths
˚
and 1–2◦.
12 (a) L. Zelikovich, J. Libman and A. Shanzer, Nature, 1995, 374,
790; (b) C. Westermeier, H.-C. Gallmeier, M. Komma and J. Daub,
Chem. Commun., 1999, 2427; (c) G. Beer, C. Niederalt, S. Grimme
and J. Daub, Angew. Chem., Int. Ed., 2000, 39, 3252; (d) A. Rajca,
A. Safronov, S. Rajca and J. Wongsriratanakul, J. Am. Chem. Soc.,
2000, 122, 3351; (e) J. Nishida, T. Suzuki, M. Ohkita and T. Tsuji,
Angew. Chem., Int. Ed., 2001, 40, 3251; (f) T. Suzuki, R. Yamamoto,
H. Higuchi, E. Hirota, M. Ohkita and T. Tsuji, J. Chem. Soc., Perkin
Trans. 2, 2002, 1937; (g) H. Higuchi, K. Ichioka, H. Kawai, K.
Fujiwara, M. Ohkita, T. Tsuji and T. Suzuki, Tetrahedron Lett., 2004,
45, 3027.
Crystal data for rac-9c chloroform solvate. C50H32N3Cl6, M
¯
893.52, colorless rod, 0.3 × 0.3 × 0.3 mm, triclinic P1, a =
˚
11.209(4), b = 12.480(5), c = 16.557(7) A, a = 86.02(1), b
◦
3
˚
= 89.83(1), c = 64.63(1) , V = 2088.6(1) A , q(Z = 2) =
1.421 g cm−1. A total of 8353 unique data (2hmax = 55◦) were
measured at T = 293 K by a Rigaku Mercury CCD apparatus
˚
(Mo-Ka radiation, k = 0.71069 A, 50 kV, 200 mA). Absorption
correction was applied (l = 4.55 cm−1). The structure was solved
by the direct method (SIR92) and refined by the full-matrix least-
squares method on F2 (all data) with anisotropic temperature
factors for non-hydrogen atoms. Hydrogen atoms were located
13 H. Kurata, T. Shimoyama, K. Matsumoto, T. Kawase and M. Oda,
Bull. Chem. Soc. Jpn., 2001, 74, 1327.
O r g . B i o m o l . C h e m . , 2 0 0 5 , 3 , 3 0 2 4 – 3 0 3 1
3 0 3 1