D. Wçll, U. E. Steiner et al.
Table 1. Quantum yields (f), light sensitivities (ef), and nucleoside
yields (YNucl) of protected nucleosides for irradiation in deaerated metha-
nol.
assigned to the HPLC chromatograms: the free nucleoside
at retention times of approximately 8 min, nitroso product 1
at retention times slightly earlier than the protected nucleo-
sides, nitroso product 2 at approximately 21 min, and the
styrene product at approximately 24 min. Because nitroso
product 2 and the styrene product are independent of the in-
itial protected nucleoside, their UV-visible spectra are iden-
tical in all cases. In contrast, the UV-visible spectrum of ni-
troso product 1 shows a signature of the investigated nucleo-
side.
Irradiation at 366 nm
Irradiation at 405 nm
Compound
f
ef[a]
YNucl
f
ef[a]
YNucl
NPPOC-Thy
0.41
0.18
0.21
0.21
0.08
0.42
0.09
0.26
0.29
0.36
100
690
820
800
250
1500
360
2100
2400
2900
920
0.90
0.60
0.75
0.86
0.27
0.21
0.92
0.66
0.61
0.52
0.52
0.41
0.09
0.14
0.14
0.05
0.38
0.09
0.27
0.23580
0.24
0.06
7
T7S2-O(CO)Thy
T7S3-O(CO)Thy
T7S4-O(CO)Thy
T7D4-O(CO)Thy
T7T4-O(CO)Thy
T4E2-O(CO)Thy
T7S0-O(CO)Thy
T7S0-O(CO)CytAc
T7S0-O(CO)AdeBz
160
320
320
170
1000
160
650
0.63
580
160
0.63
0.79
0.75
0.38
0.33
0.82
0.89
The light sensitivity of protected deoxyguanosine amidite
is less than half of the value of the other protected nucleo-
sides, as shown in Figure 3and Table 1. The reason for this
0.54
0.64
T7S0-O(CO)GuaAm 0.11
[a] in mꢀ1 cmꢀ1
because diode lasers at this wavelength have become com-
mercially available.
Whereas the increase in e is the determining factor in the
sensitivity gain by the introduction of an antenna molecule,
a general decrease in the photochemical quantum yield
could not be avoided, but was kept within a modest range of
1
about a factor of = relative to direct excitation of NPPOC.
2
(T7D4-OR and T7T4-OR should not be considered because
other photochemical primary reactions, which do not lead to
a release of the protected substrate, must also be taken into
account; see below). It is not yet clear, whether the reduc-
tion in quantum yield is due to a lower efficiency of forma-
tion of the aci-nitro intermediate or to an increased reversi-
bility of the formation of this species. This question must be
left open for further studies. The photochemical quantum
yields are fairly independent of the excitation wavelength
Figure 3. Decay kinetics of thioxanthone/NPPOC-protected nucleosides
under continuous irradiation at 366 nm. The lines represent kinetic fits
according to Equation (1).
except for compounds T7Sn-O(CO)Thy with short aliphatic
1
linkers (n=2 to 4), for which a drop by a factor of = is ob-
2
served between 366 and 405 nm.
is a decrease in the deprotection quantum yield due to com-
peting electron transfer from the deoxyguanosine to the
thioACHTRExUNG anthone moiety. This electron transfer is reversible and
For practical purposes, the total yield of release of depro-
tected substrate is at least as important as the light sensitivi-
ty. With the new compounds, these yields are between 52
and 92%. It should be noted, however, that under reaction
conditions for the synthesis of DNA chips, the yields can be
different and, of course, reaction conditions can be further
optimized for maximizing this quantity. For example, the
yield of thymidine release from NPPOC protected thymi-
dines has been reported to be as high as 98% on a chip,[25]
whereas under the conditions of our experiments the yield is
only 90%.
Experiments with other nucleosides: Thymidine has
served as the standard nucleoside for most of our investiga-
tions. To demonstrate the principal suitability of the new
type of antenna bearing protecting groups, the T7S0 conju-
gates were also synthesized for deoxyadenosine, deoxycyti-
dine, and deoxyguanosine, which also have a further protect-
ing group at their amino position (for structures, see
Scheme 2). The products formed after irradiation were simi-
lar for all nucleosides (see Figures S8–S11 in the Supporting
Information). The structures of the four main products are
results in a recovery of the reactants. Experiments for inter-
molecular quenching of thioxanthone by deoxyguanosine
amidite gave a bimolecular rate constant of 2.3109 mꢀ1 sꢀ1
(see the Supporting Information).
Due to the reduced quantum efficiency for the deprotec-
tion of deoxyguanosine amidite, the gain in light sensitivity
when using the new photolabile protecting groups is less
pronounced than for the other nucleosides. However, we be-
lieve that by using a different protecting group for the gua-
nine amino function, the oxidation potential of the nucleo-
side could be reduced and thus, electron transfer would be
avoided or at least reduced in its efficiency.
Photokinetics of the T7D4-group: In the case of the
T7D4 group, energy transfer to the NPPOC chromophore
and subsequent photorelease of the substrate has to com-
pete with a very efficient photochemical trans/cis isomeriza-
tion. The situation is described in Scheme 3.
The time profiles of the species observed when irradiating
T7D4-O(CO)Thy is shown in Figure 4.
6494
ꢀ 2008 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
Chem. Eur. J. 2008, 14, 6490 – 6497