absorbance at 425 nm (maximum naphthalene triplet forma-
tion), and R ) constant.
in the cisoid dyad, as previously observed for thymine
analogues.10 The same trend was observed for 5′-KP-dG and
5′-KP-8-oxodA, whose decays also occurred in the submi-
crosecond range.
Operating in this way, the values determined for the KP
triplet lifetimes in the dyads were 30 ns for 5′-KP-dA, 9 ns
for 5′-KP-dG, and 12 ns for 5′-KP-8-oxodA. On the basis
of these results, estimation of the involved rate constants
was made using eq 2
Thus, in the 5′-dyads, the intramolecular interaction
between KP and the purine base resulted in a significant
quenching of the excited BP-like triplet state. This could in
principle be associated with an electron transfer process;
however, the charge separated species were not detected
under the employed experimental conditions, probably due
to a very fast back electron transfer. To stabilize such species
and to enhance the prospects of detecting the purported
intermediates, water was added to the system. As a matter
of fact, laser flash photolysis (LFP) of acetonitrile-water
solutions (4:1 v/v) of 5′-KP-dA, 5′-KP-dG, and 5′-KP-8-
oxodA yielded new transients with maxima at 550 nm
(Figure 2), assigned to the characteristic BP-ketyl radical
kintra ) (1 ⁄ τT - 1 ⁄ τ0)
(2)
where kintra ) intramolecular quenching rate constant, τ0 )
triplet lifetime of free KP, and τT ) triplet lifetime in the
dyads. The values obtained (3.3 × 107 s-1, 1.1 × 108 s-1,
and 8.3 × 107 s-1 for 5′-KP-dA, 5′-KP-dG, and 5′-KP-8-
oxodA) are in agreement with the expectations for an electron
transfer mechanism. Thus, to demonstrate the viability of
the process, the free energy changes (∆G, kJ/mol) were
calculated using the Rehm-Weller eq 3
∆G ) 96.5[E0(D+• ⁄ D) - E0(A ⁄ A-•)] - ∆Eoo
(3)
where E0(D+•/D) is the one-electron oxidation potential of
the nucleobases; E0(A/A-•) is the one-electron reduction
potential of the photosensitizer, and ∆Eoo is the triplet
excited-state energy (KP or BP), determined by spectroscopic
measurements. In this context, negative ∆G increments for
the intermolecular process in related D/A systems have been
reported by Lhiaubet et al.13 for dA (∆G ) -59 kJ/mol, E0
) 1.18 V vs SCE) and dG (∆G ) -71 kJ/mol, E0 ) 1.05
V vs SCE) nucleosides, when S-KP was used as an acceptor
(E0 ) -1.24 V vs SCE, ∆Eoo ) 292.6 kJ/mol) in aqueous
media. These findings are consistent with our results for
dyads 1a, 2, and 3 by laser flash photolysis. Even though no
E0 values were available for 3, it can be assumed that the
relative free energy changes would be dG > 8-oxodA >
dA, in accordance with the nucleoside reactivities.
For the same donor-acceptor pair, the electron transfer
process should be sensitive to the length of the spacer. To
evaluate the influence of this factor, 5′-KPGly-dA was
studied by time-resolved experiments under the same condi-
tions. The transient absorption spectrum displayed the two
typical T-T bands with maxima at 330 and 530 nm (see
pages S18-S19 in Supporting Information). Its lifetime (0.4
µs) was much longer than that of 5′-KP-dA (0.03 µs), and
the rate constant determined by application of eq 2 was
accordingly lower (2.2 × 106 s-1). This constitutes a further
support for the proposed electron transfer mechanism.
Scheme 2 summarizes the sequential steps leading from the
dyads to the final 2-deoxyribonolactone product. Here,
deprotonation of the purine radical cation at C1′ could be
achieved by the BP-like radical anion. Assistance of the
aqueous medium seems to be esential, as otherwise the ketyl
radical could not reach C1′. The (KP)•- absorption (630 nm)
was not observed in the nanosecond time scale. However,
the corresponding (KPH)• band (550 nm) was clearly detected
in the LFP experiments. Previously, Cadet and co-workers
have isolated dL after UVA irradiation of 2′-deoxyguanosine
(dG) in the presence of BP, and its formation has been
attributed to photochemical electron transfer, followed by
deprotonation of the radical cation at the C1′ position. The
Figure 2. Transient absorption spectra of 5′-KP-dA (sOs), 5′-
KP-dG (sbs), and 5′-KP-8-oxodA (s9s) in acetonitrile-water
solutions, 30 ns after the 308 nm laser pulse.
moieties.11 At very early stages (<30 ns), the KP triplet
excited states were also detected, although the features of
the BP-ketyl radicals were already present. Expectedly, the
use of mixed organic-aqueous media also increased the
electron transfer efficiency, thus shortening the triplet
lifetimes.
Hence, to obtain an accurate measurement of the τT values,
the naphthalene (NP) quenching method developed by
Scaiano was employed.12 When increasing amounts of NP
were added to the dyads, deactivation of the KP triplet
excited state (selectively excited at 355 nm) was ac-
companied by generation of the NP triplet at 425 nm. A
double reciprocal plot of the absorbance increment (∆A425
)
against NP concentration (Supporting Information, see pages
S17-S18) provided the τT values upon application of eq 1
1 ⁄ ∆A425 ) R + (R ⁄ kqτT)[NP]-1
(1)
where kq ) intermolecular rate constant for quenching of
KP by NP (4 × 109 M-1 s-1), ∆A425 ) end of pulse
(11) Bensasson, R.; Gramain, J. C. J. Chem. Soc., Faraday Trans. I
1980, 76, 1801–1810.
(12) Scaiano, J. C.; McGimpsey, W. G.; Leigh, W. J.; Jakobs, S. J. Org.
Chem. 1987, 52, 4540–4544.
(13) Lhiaubet, V.; Paillous, N.; Chouini-Lalanne, N. Photochem. Pho-
tobiol. 2001, 74, 670–678.
Org. Lett., Vol. 10, No. 20, 2008
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