Quinonoid Species from 5,6-Hydroxyindole Dimers
A R T I C L E S
Br2•- was estimated to be k ) 9 × 10 M s-1. The extinction
7
-1
(TDDFT)31 approach both in vacuo and in aqueous solution,
22
coefficient of the semiquinone at 480 nm was calculated to be
using the large 6-311++G(2d,2p) basis set. Previously, a DFT
analysis of five oxidized 5,6-dihydroxyindole dimers was
reported, using both local density approximation (LDA) and
generalized gradient approximation (GGA) functionals. In that
study, however, only doubly quinonoid structures, viz., at an
oxidation state two electrons higher than those described in the
present study, were considered. In particular two conformers
of a 3,7′-biindolyl system as yet devoid of experimental support
were investigated.
4
-1
-1
4
.0 × 10 M cm .
The transient species decayed by second-order kinetics (2k
9
-1 -1
)
3 × 10 M s ) to a species with a broad band centered at
4 -1 -1
5
70 nm (ꢀ ) 9.0 × 10 M cm ) and a shoulder at 520 nm.
The isosbestic point at 500 nm denoted direct conversion of
the first species to the bathochromically shifted chromophore.
It may be noted that the spectrum of the relatively stable species
formed from the decay of the semiquinone of 2 is closely similar
to that of melanochrome observed in the metal-catalyzed
oxidation of 2.26 Indeed, the species may well be identical.
Figures 3 and 4 indicate that 3 and 4 behaved quite differently
from 2. Dimer 3 gave a semiquinone (λmax ) 460 nm, ꢀ ) 11700
For the purposes of the present study, we chose to use the
“hybrid” PBE0 functional, which has been shown to provide
quite satisfactory energies and geometries for a wide range of
3
2
organic and biological systems, as well as a rather accurate
-
1
-1
9
-1
33
M
cm ) with a formation rate constant k ) 1.8 × 10 M
description of low-lying excited states. To assess the perfor-
-1
s . The semiquinone(s) apparently decayed with second-order
mance of the selected DFT technique in predicting electronic
absorption spectra of dimeric quinones, test calculations were
carried out on simple benzoquinones/benzoquinone imines, and
on indigo, a prototypical conjugated indole dimer. Overall, the
results (see the Supporting Information) confirmed that the
method chosen is capable of reproducing the UV-vis spectra
of such chromophores with reasonable accuracy. Thus, for
example, if one focuses on the most intense transitions, the
predicted wavelength for p-benzoquinone in vacuo is 247 nm,
to compare with an experimental value of 240 nm. For
p-benzoquinonimine (in water) the computed transition is at 266
nm, while the experimental spectrum shows a split band with
maxima at 260 and 254 nm. The related N-phenyl-p-benzo-
quinonimine in methanol has strong transitions at 490, 309, and
267 nm, in fair agreement with the experimental values of 448,
285, and 263 nm. A comparable error is obtained in the case of
indigo (computed 570 nm, measured 600 nm).
9
-1 -1
kinetics (2k ) 2.8 × 10 M s ), resulting in the generation
of species with broad bands at 490 nm (ꢀ ) 17700 M cm )
and at 530 nm (ꢀ ) 15900 M cm ). Dimer 4 gave a
-
1
-1
-
1
-1
9
-1 -1
semiquinone (formation rate constant k ) 2.2 × 10 M s )
with a broader, seemingly split band (λmax ) 430 nm, ꢀ ) 8.6
3
-1
-1
3
-1
-1
×
10 M cm , and 480 nm, ꢀ ) 8.1 × 10 M cm ). The
semiquinone(s) decayed with second-order rate constants 2k )
9
-1 -1
9
1
M
.4 × 10 M
s
measured at 480 nm and 2k ) 2.1 × 10
-
1
-1
s
determined at 430 nm. Concomitant to semiquinone
decay, a chromophore developed with a broad maximum
centered around 530 nm. If it is assumed that a single
semiquinone species is responsible for the bands at 420 and
4
80 nm, then the extinction coefficient of the quinone can be
-1
-1
calculated to be 11100 M cm at 530 nm taking as reference
the semiquinone band at 480 nm. If there is more than one
quinone, such a calculation is invalid. Overall, these pulse
radiolysis studies suggested that oxidation of 2-4 leads to the
generation of semiquinone intermediates which decay by a
bimolecular process. This may consist of either disproportion-
ation, to give two-electron oxidation products generically
referred to as “quinones”, or dimerization, to afford tetraindolyl
species. To address this issue, a theoretical investigation of the
main tautomeric forms of quinones from dimers 2-4 was
undertaken.
Theoretical Studies and Simulated Electronic Absorption
Spectra of Biindolyl Quinone Tautomers. Pairs of syn-
periplanar (sp) and anti-periplanar (ap) rotamers can be envis-
aged for the o-quinone, quinone methide, and quinonimine
tautomers of dimers 2-4, depending on the orientation of the
indole rings around the single bond, whereas two geometrical
isomers (E and Z) are possible for the extended forms. To
determine which of these structures may be a plausible candidate
for the observed two-electron oxidation products of the dimers,
The molecular structures of the main quinone tautomers for
dimer 2 along with their relative energies are shown in Figure
5; a complete listing of the structures examined is presented in
the Supporting Information.
DFT results suggest that the extended forms 2a and 2b are
by far the most stable tautomers in the series. The structures
that come next, namely, methides 2c and 2d in vacuo, and
quinone 2g in aqueous solution, are separated by several
kilocalories per mole. Interestingly, in vacuo the E isomer 2b
is planar and slightly more stable than the Z isomer 2a, in which
the indole rings are twisted by 3.4°. However, in aqueous
solution both isomers are planar and the E isomer is destabilized
-
1
by ca. 1.1 kcal mol . With respect to all other tautomers, the
o-quinone tautomers feature one less intramolecular OH-O
hydrogen bond. Thus, their relative stability increases signifi-
(
31) (a) Stratmann, R. E.; Scuseria, G. E.; Frisch, M. J. J. Chem. Phys. 1998,
1
09, 8218-8224. (b) Bauernschmitt, R.; Ahlrichs, R. Chem. Phys. Lett.
all tautomeric quinones of dimers 2-4 were geometry-optimized
1996, 256, 454-464. (c) Casida, M. E.; Jamorski, C.; Casida, K. C.;
Salahub, D. R. J. Chem. Phys. 1998, 108, 4439-4449. (d) Adamo, C.;
Scuseria, G. E.; Barone, V. J. Chem. Phys. 1999, 111, 2889-2899.
in vacuo at the PBE0/6-31+G(d,p) level of theory.29 For each
-
1
dimer, all structures that were within ca. 15 kcal mol from
the minimum-energy structure were also optimized using the
polarizable continuum model (PCM)30 to simulate the aqueous
environment; the absorption spectra of all the energetically
relevant species were computed using the time-dependent DFT
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(
b) Benzi, C.; Improta, R.; Scalmani, G.; Barone, V. J. Comput. Chem.
2
002, 23, 341-350. (c) Langella, E.; Rega, N.; Improta, R.; Crescenzi,
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1
24, 7857-7865.
(33) (a) Jacquemin, D.; Wathelet, V.; Perpete, E. A. J. Phys. Chem. A 2006,
10, 9145-9152. (b) Preat, J.; Jacquemin, D.; Wathelet, V.; Andre, J.-M.;
1
Perpete, E. A. J. Phys. Chem. A 2006, 110, 8144-8150. (c) Jacquemin,
D.; Preat, J.; Wathelet, V.; Fontaine, M.; Perpete, E. A. J. Am. Chem. Soc.
2006, 128, 2072-2083. (d) Crescenzi, O.; Pavone, M.; De Angelis, F.;
Barone, V. J. Phys. Chem. B 2005, 109, 445-453. (e) Aquilante, F.; Cossi,
M.; Crescenzi, O.; Scalmani, G.; Barone, V. Mol. Phys. 2003, 101, 1945-
1953. (f) Adamo, C.; Barone, V. Chem. Phys. Lett. 2000, 330, 152-160.
(
29) Adamo, C.; Barone, V. J. Chem. Phys. 1999, 110, 6158-6170.
(
30) (a) Miertus, S.; Scrocco, E.; Tomasi, J. Chem. Phys. 1981, 55, 117-129.
(
b) Cossi, M.; Scalmani, G.; Rega, N.; Barone, V. J. Chem. Phys. 2002,
1
17, 43-54. (c) Scalmani, G.; Barone, V.; Kudin, K. N.; Pomelli, C. S.;
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J. AM. CHEM. SOC.
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VOL. 128, NO. 48, 2006 15493