˚
(2.9–3.3 A). Such an arrangement brings to mind the possibility
twisting of the methylated derivatives (8 and 9) nor the proximity
of chromophores in 3 lead to any statistically relevant deviation
in the quantum efficiency.
of ring-closure of a suitable precursor to an [8]circulene type
structure, with alternating six- and five-membered rings.
The distortion of 3 from D2h (planar) to C2 (ground state)
gives rise to the possibility of dynamic behavior. The two
possible dynamic modes of interest are the inversion of the
core eight-membered ring through the plane and the twisting
of the fluoranthene subunit. The former process is highly
unlikely at room temperature, for example, an exceptional
Acknowledgements
This work was supported by the US National Science Founda-
tion, the Swiss National Science Foundation, and the Japanese
Society for the Promotion of Science.
thermal racemization barrier of 67.2
0.8 kcal mol−1 was
measured for dibenzo[b,h]tetraphenylene.10 The barrier to ring-
inversion for tetraphenylene derivatives is commonly between
25 and 45 kcal mol−1,11,12 thus, the central ring is essentially
locked in place. In 3, the twisting of the fluoranthene subunits
should occur with a much lower barrier, either stepwise, among
diastereomeric complexes, or correlated between enantiomers
through an effective C2v transition form.
The methyl groups of 3 appear as only a single set of signals
in the proton NMR, expressing the time-averaged symmetry of
the dynamically twisting racemate. If a frozen solution structure
akin to that seen in the X-ray crystal structure could be obtained,
two sets of methyl signals, exo and endo, should be seen. This
would only be observable at lower temperatures.
Notes and references
† CCDC reference number 255954. See http://www.rsc.org/suppdata/
ob/b4/b416820h/ for crystallographic data in .cif format. Crystal
data 3 (0.30 × 0.20 × 0.10 mm3): Formula C52H40; formula weight
˚
664.84; crystal system monoclinic;◦ a = 17.705(2) A, b = 21.289(2)
3
˚
˚
˚
A, c = 19.354(2) A, b = 96.336(3) , V = 7250.4(15) A , T = 296(2)
K; space group C2/c; Z = 8; m = 0.069 mm−1; q = 1.218 mg
m−3; reflections collected 18208; independent reflections 6303 [R(int) =
0.0306]; data/restraints/parameters 6303/0/477; goodness of fit on F2
0.875; final R indices [I > 2r(I)] R1 = 0.0401, wR2 = 0.0997; R indices
(all data) R1 = 0.0693, wR2 = 0.1080; largest diff. peak and hole 0.126
−3
˚
and −0.134 e A
.
1 R. G. Harvey, Polycyclic Aromatic Hydrocarbons, Wiley-VCH, New
York, NY, 1997.
In an attempt to measure the barrier to twisting in 3, dynamic
2 (a) G. N. Sastry, Curr. Sci., 2003, 85, 125; (b) D. T. Colbert and
R. E. Smalley in Perspectives of Fullerene Nanotechnology, ed.
E. Osawa, Kluwer Academic Publishers, Dordrecht, Amsterdam,
2002, 3; (c) K. K. Baldridge and J. S. Siegel, Theor. Chem. Acc., 1997,
97, 67; (d) H. Sakurai, T. Daiko and T. Hirao, Science, 2003, 301,
1878; (e) T. J. Seiders, E. L. Elliott, G. H. Grube and J. S. Siegel,
J. Am. Chem. Soc., 1999, 121, 7804; (f) L. T. Scott, P.-C. Cheng,
M. M. Hashemi, M. S. Bratcher, D. T. Meyer and H. B. Warren,
J. Am. Chem. Soc., 1997, 119, 10963.
1H-NMR spectra were recorded at temperatures from −120 to
◦
25 C in dichlorofluoromethane-d.13 However, no splitting of
the signal set was observed, implying an upper limit to the
twisting barrier of ca. 7.5 kcal mol−1. This conclusion is given
additional support by the recently reported barrier to twisting of
8,9-diacetoxy-1,6,7,10-tetramethylfluoranthene (DG‡ < 7.0 kcal
mol−1).9
Luminescence was observed during the isolation of 3. This
is not surprising given the fluorescent properties of the parent
fluoranthene (7), however, perturbations of the electronic spectra
of 3 could reveal something about the coupling between
the juxtaposed chromophores. Thus, it was decided to study
the photophysics of the series of fluoranthenes: 8,9-diphenyl-
1,6,7,10-tetramethylfluoranthene (9),14 and 3.
3 K. Yamamoto, T. Harada, M. Nakazaki, T. Naka, Y. Kai, S. Harada
and N. Kasai, J. Am. Chem. Soc., 1983, 105, 7171.
4 D. N. Leach and J. A. Reiss, J. Org. Chem., 1978, 43, 2484.
5 E. Clar, R. Schoental, Polycyclic Hydrocarbons; Academic Press,
New York, ch. 1, 1964.
6 (a) A. Orita, D. Hasegawa, T. Nakano and J. Otera, Chem. Eur. J.,
2002, 8, 2000; (b) For the original report of 4 see: H. N. C. Wong,
P. J. Garratt and F. Sondheimer, J. Am. Chem. Soc., 1974, 96, 5604.
7 R. Destro, T. Pilati and M. Simonetta, J. Am. Chem. Soc., 1975, 97,
658.
8 1,6,7,12,13,18,19,24-Octamethylacenaphthyleno[b,l]tetraphenylene
(3). 6,7-Dihydro-6-hydroxy-7,9-dimethyl-8H-cyclopenta[a]acena-
phthylene-8-one (6) (440 mg, 1.58 mmol) and 5,6,11,12-
tetradehydrodibenzo[a,e]cyclooctene (4) (79 mg, 0.40 mmol)
were dissolved in acetic anhydride (20 mL) under an argon
atmosphere. The suspension was heated to 100 ◦C and gently
stirred for 12 h. The resulting solution was cooled to ambient
temperature, diluted with toluene (20 mL) and quenched slowly
with 2 M NaOH. The organic layer was washed three times with
additional 2 M NaOH (50 mL), dried over MgSO4 and then passed
through a short plug of silica gel. The crude product was purified
by column chromatography on silica gel with 5% ethylacetate in
hexane as the eluent to yield an orange solid (210 mg, 78%). Mp
354 ◦C (d). 1H NMR (CDCl3, 500 MHz), ppm: 2.47 (s, 12H), 2.70 (s,
12H), 7.21–7.26 (m, 8H), 7.29 (d, 3J = 8, 4H), 7.61 (d, 3J = 8, 4H)
13C NMR (CDCl3, 125 MHz), ppm: 22.5, 24.9, 126, 126.5, 126.53,
126.7, 129.7, 131.69, 131.72, 134, 135.1, 139.7, 141.6. UV (CH3CN)
The UV kmax displays a predictable red shift upon methyl
or phenyl substitution (Table 1) concomitant with twisting of
the plane. Somewhat surprising is the lack of any significant
differences among 8, 9, and 3, however, the severely distorted
central ring prevents conjugation, and allows the two fluo-
ranthene substructures to behave like isolated units. The only
noticeable change is a slight increase in molar absorptivity. The
change in the fluorescent emission throughout the series is one
of spectral structure rather than wavelength. The parent displays
two maxima, but only the longer wavelength emission persists
in 8, 9, and 3. The quantum efficiencies (φf ) were measured by
comparison to 9,10-diphenylanthracene in cyclohexane15 and
are the same, within experimental error. Thus, neither the severe
l
max, nm (e): 250 (7 × 104), 277 (4 × 104), 288 (4 × 104), 298 (4 ×
104), 338 (1 × 104), 373 (2 × 104). HRMS: found 664.3155, calcd.
(C52H40) 664.3130.
9 A. Borchardt, K. Hardcastle, P. Gantzel and J. S. Siegel, Tetrahedron
Lett., 1993, 34, 273.
10 P. Rashidi-Ranjbar, Y. M. Man, J. Sandstrøm and H. N. C. Wong,
J. Org. Chem., 1989, 54, 4888.
11 A. Rosdahl and J. Sandstrøm, Tetrahedron Lett., 1972, 4187.
12 G. H. Senkler, Jr., D. Gust, P. K. Riccobono and K. Mislow, J. Am.
Chem. Soc., 1972, 94, 8626.
Table 1 Photophyscial properties of 3 and 7–9
13 J. S. Siegel and F. A. L. Anet, J. Org. Chem., 1988, 53, 2629.
14 8,9-Diphenyl-1,6,7,10-tetramethylfluoranthene (9). 6,7-Dihydro-
6-hydroxy-7,9-dimethyl-8H-cyclopenta[a]acenaphthylene-8-one (6)
(552 mg, 2.0 mmol) and diphenylacetylene (373 mg, 2.1 mmol) were
dissolved in acetic anhydride (20 mL) under an argon atmosphere.
The suspension was heated to reflux and gently stirred for 3 d. The
resulting solution was cooled to ambient temperature, diluted with
toluene (20 mL) and quenched slowly with 2 M NaOH. The organic
kmax/nm
kem/nm
φf
7
8
9
3
358
369
374
373
431, 455
452
458
0.20 0.02
0.19 0.02
0.21 0.03
0.17 0.02
461
5 8 2
O r g . B i o m o l . C h e m . , 2 0 0 4 , 3 , 5 8 1 – 5 8 3