Abstract:
Nanoporous Titanium dioxide (TiO2) combined with poly (3-hexylthiophene) polymer is a promising
nanocomposite for cost efficient photovoltaic devices. However, the poor power conversion efficiency
found in such devices is mainly attributed to the lower chemical compatibility between the metal
oxide and polymer. As such,it causes poor polymer penetration in to highly-structured nanoporous
TiO2. More recently, we have shown that polymer penetration can be improved by coating the
nanoporous TiO2. We further showed that hole-mobility of the polymer can also be improved by
modifying the nanoporous TiO2 with dye over layer.
In this work,monolayer of commercially available and widely used ruthenium (Ru) based dye,
N719,and a newly synthesized[Ru(bpy)2(dcbpy)][PF6]2 (bpy = 2,2’-bipyridine; dcbpy = 4,4’-
dicarboxy-2,2’-bipyridine)dye (RuC2)were introduced at the TiO2 / P3HT interface,and their effect in
photovoltaic parameters were examined.
RuC2 dye adsorption on nanoporous TiO2 electrode is higher than other Ru based dyes studied. This
is probably due to its chemical structures; the N719 dye consist NCSisothiocyanatefunctional group
along with carboxylic acid (COOH)substituted two biphenyl rings, whereas the newly synthesized dye
contains three biphenyl rings with two COOH groups, which can bind easily to TiO2due to less steric
hindrance. Nanoporous TiO2 films treated with these dyes showed a very weak optical absorption in
the visible region in comparison with the absorption of the polymer used in this study. Quantum
efficiency spectra of both control and dye coated devices show that dyes has no contribution in
creating of carriers for device current, but the dye serves as interface modifier.RuC2 dye treated
devices showed a 75 % of enhancement in the power conversion efficiency compared to the devices
treated with the commercial (N719) dye, mainly due to increase in short circuit current density. This
is attributed due to better interaction between RuC2 and TiO2as well as lower laying LUMO of
synthesized RuC2 dye which enables an easy electron transfer cascade from P3HT to the RuC2
interface layer to TiO2 and, thereby, potentially enhancing charge separation at the TiO2
interface. Additionally, on account of the deep HOMO level of RuC2 relative to P3HT, the RuC2
layer is expected to obstruct hole-transfer between P3HT and TiO2, and thus to localize hole-polarons
in the P3HT away from the TiO2 surface.