heterocyclic nitrogen containing acceptor for metal-free D-p-A
DSC dyes. The acceptors presented in this work offer a range of
withdrawing strengths for maximizing color and injection efficiency
based on E(S+/S*). These efficient acceptors include two hetero-
cycles, pyridine and pyrazine, with less withdrawing strength than
cyanoacrylate and one heterocycle, quinoxaline, with more with-
drawing strength. The carboxylate anchored pyrazine acceptor
used in JD7 and the pyridine acceptor used in dye JD2 demon-
strate excellent charge separation and efficient charge injection.
These acceptors will likely find future application for dye design
involving p-bridge chromophores where E(S+/S*) is already too low
for the addition of a strongly withdrawn cyanoacrylate. In this
case, both pyridine and pyrazine acceptors would provide a dipole
for photon induced charge separation and a better driving force for
injection by generating a smaller shift with respect to the E(S+/S*)
level than cyanoacrylate. Furthermore, dye JD7 is a promising
dye for co-sensitized DSC devices due to a strong IPCE from
400–550 nm (near 90%) and no need for the addition of
CDCA to diminish aggregation.
Fig. 2 Current versus potential plot for dyes JD2, JD4, JD7 and JD8.
in Voc is observed for devices with JD7 and CDCA. All the
devices tested (with or without CDCA) give substantially
lower voltage than JD7 which can in part be attributed to
the difference in dye loading since higher loadings aid in
blocking potential recombination sites with the electrolyte and
semiconductor surface (see ESIw). Comparatively, JD2 has
significantly less absorbance in the visible region which leads
to a lower Jsc of 7.87 mA cmꢀ2 and an optimized PCE of 4.05%
in the presence of CDCA (Table 2). JD2 is the most strongly
affected dye with respect to the benefits of CDCA and displays
an increase in both current and voltage when compared to
solutions with no co-adsorbent. JD8 shows an increase in
voltage with the addition of CDCA and a loss of current.
JD8 suffers from a decreased driving force for injection, lower
dye loading and aggregation (see ESIw). In all cases except
devices with JD7, lack of CDCA addition to the dye solutions
led to diminished photovoltaic performance. Dye aggregation
likely causes intermolecular energy transfer and subsequently
results in excited-state quenching of the dyes.
We would like to acknowledge ERC-ARG and the
FP7-Energy-2010-FET project Molesol (Contract No. 256617)
for financial support.
Notes and references
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c
This journal is The Royal Society of Chemistry 2012
Chem. Commun., 2012, 48, 2295–2297 2297