rality method2c,h,7 with respect to the two TPP(Zn) (tet-
raphenylporphyrin zinc complex) adducts (see the Supporting
Information). As the number of naphthalene units increased,
the solubility decreased. Among the diastereomers, alternat-
ing-chiral naphthalenes with the oxy-functional groups
concentrated on one side were less soluble because the dipole
moment of the entire molecule is larger than that of the other
diastereomers. Octamer 10 was the upper limit without
solubilizing substituted groups. These methylenedioxy bridges
were stable under heat, at least up to 80 °C, as well as under
moderate acidic or basic conditions. Moreover, epimerization
did not occur under these conditions.8
nm) became broader and the spectra was red-shifted, while
the change in the maximum absorption wavelength of the
short wavelength side (220-240 nm) was insignificant. These
results indicate that 1La (transition moment of the short axes
of the naphthalene rings) rather than 1Bb (transition moment
of the long axes of the naphthalene rings) is affected,9 and
adjacent naphthalene rings interact strongly in the rod
direction. Each diastereomer displayed similar characteristics,
but the spectral shape varied slightly (Figure S2, Supporting
Information). Open-form compounds 1, which are even
higher order oligonaphthalenes, did not exhibit a red-shift.2a,g
In Figure 2B, the CD intensity of (R)-6 was much higher
than that of (R)-5, although both had identical Cotton effect
patterns. Moreover, debenzylated analogues of (R)-6 showed
similar spectra (Figure S4, Supporting Information). There-
fore, the optical properties directly reflect differences in the
torsion angle of the naphthalene rings. Higher order (R,S,R)-8
and (R,S,R,S,R,S,R)-10 had CD intensities almost identical
to that of (R)-6. Because each naphthalene ring of 8 and 10
interacted with distant naphthalene rings, the CDs of S and
R binaphthalene units canceled each other on a whole. Figure
2C shows the emission spectra in solution. Along with the
absorption, the emission shifted bathochromically with the
number of naphthalene rings. Each compound showed rela-
tively high FL quantum yields in solution; φ310 of (R)-6 was
0.44, φ330 of (R,S,R)-8 was 0.79, and φ330 of (R,S,R,S,R,S,R)-
10 was 0.64. In contrast, φfl of the open-form dimers was
relatively low; φ310 of (R)-5 was 0.045,10 and φ310 for
compounds with methoxy groups instead of hydroxy groups
of (R)-5 was 0.16. The reason that bridged oligonaphthalenes
exhibited a high fluorescence is unknown. However, plausible
explanations include that the bridges provide the entire
molecule with rigidity, especially the constraint axial rotation,
or as suggested by the relatively small Stokes shifts (for
example, the Stokes shift of (R,S,R,S,R,S,R)-10 is 36 nm),
the dihedral angles of the naphthalene rings of the S0 state
are inherently similar to that of the S1 state,11 tand hus, the
excitation energy is more likely to be converted into
fluorescence than axial vibration. Moreover, the bridged
oligonaphthalenes strongly fluoresced in the solid state under
UV light (Figure 2D, φ ) 0.08-0.21); (R)-6 was pale blue
Figure 2 depicts the optical properties. Figure 2A shows
the absorption spectra; as the number of naphthalene rings
increased, the longer wavelength absorption region (320-400
(5) Dihedral angles of the two naphthalene rings in the X-ray crystal
structure of the bridged dimers are observed slightly above 50°; see :(a)
Deussen, H.-J.; Boutton, C.; Thorup, N.; Geisler, T.; Hendrickx, E.;
Bechgaard, K.; Persoons, A.; Bju`rnholm, T. Chem.sEur. J. 1998, 4, 240.
(b) Schneider, J. F.; Nieger, M.; Na¨ttinen, K.; Lewall, B.; Niecke, E.; Do¨tz,
K. H. Eur. J. Org. Chem. 2005, 1541.
(6) Litvinchuk, S.; Bollot, G.; Mareda, J.; Som, A.; Ronan, D.; Shah,
M. R.; Perrottet, P.; Sakai, N.; Matile, S. J. Am. Chem. Soc. 2004, 126,
10067.
(7) (a) Harada, N.; Nakanishi, K. Acc. Chem. Res. 1972, 5, 257. (b)
Koslowski, A.; Sreerama, N.; Woody, R. W. In Circular Dichroism:
Principles and Applications; Berova, N., Nakanishi, K., Harada, N., Eds.;
Wiley-VCH: New York, 2000; pp 55-95.
(8) Racemization barriers of a simple compound have been reported
(∆Gq ) 33 kcal/mol in decalin), see: Park, J.-W.; Ediger, M. D.; Green,
M. M. J. Am. Chem. Soc. 2001, 123, 49.
Figure 2. Optical properties of bridged oligonaphthalene (R)-6 (red
line), (R,S,R)-8 (black line), (R,S,R,S,R,S,R)-10 (aqua line), and
nonbridged (R)-5 (green line): (A) absorption spectra in 1,4-dioxane;
(B) CD spectra in 1,4-dioxane; (C) fluorescence spectra in 1,4-
dioxane (excitation wavelengths are 310 nm for 5 and 6 and 330
nm for 8 and 10); (D) pictures of solid-state fluorescence under
UV light (254 nm).
(9) Rosini, C.; Superchi, S.; Peerlings, H. W. I.; Meijer, E. W. Eur. J.
Org. Chem. 2000, 61.
(10) Hydroxy groups of BINOL are involved in its fluorescence
quenching, see: Wang, Q.; Chen, X.; Tao, L.; Wang, L.; Xiao, D.; Yu,
X.-Q.; Pu, L. J. Org. Chem. 2007, 72, 97.
(11) Dihedral angles of the S0 and S1 state have been studied; see:
Fujiyoshi, S.; Takeuchi, S.; Tahara, T. J. Phys. Chem. A 2004, 108, 5938.
1834
Org. Lett., Vol. 12, No. 8, 2010