Chemistry Letters 2000
1373
dimer. This was accompanied with drastic conformational
changes of one of phenyl rings (the central one in Figure 1 was
rotated by 60°). The intermolecular distance between the bridg-
ing carbon atoms before irradiation was 4.87 Å. Two other imi-
dazolyl rings with a 4π-electron system moved outward (by max
References and Notes
#
Present address: Department of Applied Chemistry, Graduate School
of Engineering, Tokyo Metropolitan University, Tokyo 192-0397
G. M. J. Schmidt and M. D. Cohen, J. Chem. Soc., 1964, 1996.
M. D. Cohen, Angew. Chem., Int. Ed. Engl., 14, 386 (1975); J. M.
McBride, B. E. Segmuller, M. D. Hollingsworth, D. E. Mills, and B.
A. Weber, Science, 234, 830 (1986); J. R. Scheffer, in “Organic
Solid State Chemistry,” ed. by G. R. Desiraju, Elsevier, Amsterdam
(1987), Chap. 1; J. N. Gamlin, J. N. Gamlin, R. Jones, M. Leibovitch,
B. Patrick, J. R. Scheffer, and J. Trotter, Acc. Chem. Res., 29, 203
1
2
1
.86 Å) to form two planar lophyl radicals sandwiching the 2,2'-
dimer. On warming to 25 °C, the black crystal returned to the
initial pale-yellow HABI crystal. The black crystal was consider-
ably stable at room temperature in contrast with the irradiated
crystal of o-Cl-HABI containing lophyl radical pairs only.
(1996).
3
4
N. J. Turro, “Modern Molecular Photochemistry,” University
Science Books, Sausalito, CA (1991).
ESR spectra of a single crystal of HABI irradiated at 77 K
for 30 min showed a broad doublet signal corresponding to free
lophyl radicals at g = 2.003. Reflective visible spectra of an
irradiated KBr pellet of HABI also indicated the presence of
lophyl radicals (λmax = 566 nm). In addition, its infrared spectra
consisted of bands assigned to an unreacted 1,2'-dimer, a
Y. Ohashi, Acc. Chem. Res., 21, 268 (1988); Y. T. Osano, A.
Uchida, and Y. Ohashi, Nature, 352, 510 (1991); Y. Ohashi, Acta
Crystallogr. Sect. A, 54, 842 (1998); Y. Ohashi and Y. Sasada,
Nature, 267, 142 (1977).
5
6
7
J. Harada, H. Uekusa, and Y. Ohashi, J. Am. Chem. Soc., 121, 5809
(
1999).
M. Kawano, T. Sano, J. Abe, and Y. Ohashi, J. Am. Chem. Soc., 121,
106 (1999).
8
15
piezodimer of HABI and lophyl radicals. Figure 2 shows the
U. K. Genick, S. M. Soltis, P. Kuhn, I. L. Canestrelli, and D. E.
Getzoff, Nature, 392, 206 (1998); P. Coppens, D. V. Fomitchev, M.
D. Carducci, and K. Culp, J. Chem. Soc., Dalton Trans., 1998, 865.
M. Kawano, A. Ishikawa, Y. Morioka, H. Tomizawa, E. Miki, and
Y. Ohashi, J. Chem. Soc., Dalton Trans., 2000, 2425.
A. B. Cohen and P. Walker, in “Imaging Processes and Materials,”
Neblette’s 8th ed., ed. by J. M. Sturge, V. Walworth, and A. Shepp,
van Nostrand Reinhold, New York (1998), pp. 226–262.
8
9
1
0
K. Maeda, in “Processes in Photoreactive Polymers,” ed. by V. V.
Krongauz and A. D. Trifunac, Chapman & Hall, New York (1995),
pp. 90–110.
1
1
1
2
T. Hayashi and K. Maeda, Bull. Chem. Soc. Jpn., 33, 565 (1960).
HABI was prepared according to ref 11. A thin plate crystal (220 ×
1
40 × 20 µm) of HABI was cooled below 108 K. The 1,2'-dimer
structure of HABI was determined by X-ray diffraction involving the
use of a SMART CCD area detector diffractometry system. With
irradiation, the X-ray data showed no significant crystal decay.
–
C H N , MW = 590.70, triclinic, space group P1, T = 108(2) K, a =
42
30
4
1
1.3298(4) Å, b = 12.8275(4) Å, c = 13.0737(4) Å, α = 60.634(1)°,
3
β = 80.389(1)°, γ = 67.071(1)°, V = 1524.37(9) Å , Z = 2, d
=
calcd
3
1
.287 Mg/m . Structural solution by direct methods and anisotropic
2
least-squares refinement (based on F ) were performed with
SHELXTL (version 5.0). Anisotropic least-squares refinement (416
parameters) on 8853 independent merged reflections (Rint = 0.0439)
converged at R (F) = 0.0462 for 6009 observed data (I > 2σ(I)),
1
GOF = 1.014.
1
3
4
o-Cl-HABI indicates 2,2'-di(o-chlorophenyl)-4,4',5,5'-tetraphenyl
biimidazole. Photolysis of a crystal of o-Cl-HABI produced radical
pairs in 10% yields as reported in ref 6.
IR spectra of 1,2'-dimer (A–D) and piezodimer independently
prepared according to Reference 15. The bands with asterisks of
1
A thin plate crystal (300 × 160 × 20 µm) of HABI was cooled below
1
,2'-dimer in (A) showed salient changes on irradiation. The
1
08 K and irradiated with a high-pressure mercury lamp for 30 min.
42 30 4
–
spectrum of C indicates the appearance of piezodimers and the
decrease of 1,2'-dimer. The IR spectra of A–D show that this
photochemical process is reversible. These facts support that the
piezodimer and lophyl radicals were formed from HABI.
Although the formation of a piezodimer from HABI has been
assumed without knowledge of its structural formula, its struc-
ture has never been determined because of the difficulty in
obtaining single crystals. The recrystallization of the independ-
ently prepared piezodimers led to the formation of stable 1,2'-
dimers owing to the thermodynamical instability; a 2,2'-dimer (a
C H N , MW = 590.70, triclinic, space group P1, T = 108(2) K, a
= 11.3660(7) Å, b = 12.8563(9) Å, c = 13.085(1) Å, α = 60.638(1)°,
3
β = 80.208(1)°, γ = 66.501(1)°, V = 1527.5(2) Å , Z = 2, d
=
calcd
3
1
.287 Mg/m . During the data collection below 108 K, no decay
was observed. Isotropic and anisotropic least-squares refinement
(378 parameters/291 restraints) on 8857 independent merged reflec-
tions (Rint = 0.0783) converged at R (F) = 0.0741 for 4643 observed
1
data (I > 2σ(I)), GOF = 1.031. Refinement: Photolysis of HABI
produced three new molecular groups except the unreacted 1,2'-
dimer (63.8(8)%); that is, lophyl radicals (13.9(2)%), 2,2'-dimer
(
13.9(2)%), and another unreacted 1,2'-dimer (22.3(5)%). The minor
unreacted 1,2'-dimer was located close to the parent unreacted 1,2'-
dimer. The parent 1,2'-dimer was treated as a rigid group that was
modeled from the structural parameters in ref 12. The temperature
parameters of the parent 1,2'-dimer were fixed. The phenyl groups
of lophyl radicals and 2,2'-dimer were restrained due to severe over-
laps with those of the parent 1,2'-dimer. The crystal structure of the
minor 1,2'-dimer is omitted in Figure 1 for clarity.
4
π–4π electron system) is less stable than a 1,2'-dimer (a 4π–6π
electron system) because of lack of resonance effects in the imi-
dazolyl rings. In this study HF/6-31G calculations predicted that
–1
a 1,2'-dimer is more stable by 5.9 kcal mol than a 2,2'-dimer.
This study shows the successful application of a cryotrap-
ping method to capture light-induced unstable intermediates in
a crystal and to characterize their structures by in situ X-ray
crystallography.
15 D. M. White and J. Sonnenberg, J. Am. Chem. Soc., 88, 3825 (1966).
16
T. Shida, K. Maeda, and T. Hayashi, Bull. Chem. Soc. Jpn., 43, 652
(1970); K. Maeda and T. Hayashi, Bull. Chem. Soc. Jpn., 43, 429
(1970).
This work was supported by CREST from JST.