Porphyrin oriented self-assembled
nanostructures for efficient exciton dissociation
in high-performing organic photovoltaics†
M. Vasilopoulou,
*
a
D. G. Georgiadou,
a
A. M. Douvas,
a
A. Soultati,
a
V. Constantoudis,
a
D. Davazoglou,
a
S. Gardelis,
a
L. C. Palilis,
b
M. Fakis,
b
S. Kennou,
c
T. Lazarides,
d
A. G. Coutsolelos
d
and P. Argitis
a
Herein we report on enhanced organic solar cell performance through the incorporation of cathode
interfacial layers consisting of self-organized porphyrin nanostructures with a face-on configuration. In
particular, a water/methanol-soluble porphyrin molecule, the free base meso-tetrakis(1-
methylpyridinium-4-yl)porphyrin chloride, is employed as a novel cathode interlayer in bulk
heterojunction organic photovoltaics. It is demonstrated that the self-organization of this porphyrin
compound into aggregates in which molecules adopt a face-to-face orientation parallel to the organic
semiconducting substrate induces a large local interfacial electric field that results in a significant
enhancement of exciton dissociation. Consequently, enhanced photocurrent and open circuit voltage
were obtained resulting in overall device efficiency improvement in organic photovoltaics based on bulk
heterojunction mixtures of different polymeric donors and fullerene acceptors, regardless of the specific
combination of donor–acceptor employed. To highlight the impact of molecular orientation a second
porphyrin compound, the Zn-metallated meso-tetrakis(1-methylpyridinium-4-yl)porphyrin chloride, was
also studied and it was found that it forms aggregates with an edge-to-edge molecular configuration
inducing a smaller increase in the device performance.
1. Introduction
Organic photovoltaic (OPV) cells hold great economic potential
as they may lead to a new generation of consumer devices that
can be processed at low cost on large areas, have light weight
and conform to exible substrates.
1–3
Until now, high efficien-
cies of 7–10% have been realized in OPVs based on polymer
donor–fullerene acceptor bulk heterojunctions (BHJs), mainly
through the optimization of the bandgap and the highest
occupied molecular orbital (HOMO) level of the semiconduct-
ing polymer and the lowest unoccupied molecular orbital
(LUMO) level of the fullerene acceptor.
4–6
However, further
improvements are needed to enhance the efficiency towards the
goal of 10% and, thus, to render their mass production and
practical applications feasible. Because efficient operation of
OPVs relies on the efficient separation and collection of pho-
togenerated carriers, approaches to further increase their effi-
ciency should aim towards recovery of energy losses caused by
the interfacial energy level misalignments and the recombina-
tion of excitons.
7–9
Especially, non-radiative exciton recombi-
nation reduces (a) the charge concentration and thus, the
corresponding photocurrent and (b) the quasi-Fermi energy
difference (i.e. chemical potential) between electrons and holes,
resulting in the lowering of the open circuit voltage (V
oc
). This
process is usually invoked to explain the hitherto observed
relatively low V
oc
in most OPVs.
10,11
To date the most successful
strategies to circumvent interfacial energetic and exciton
recombination losses include, respectively, a plethora of alter-
native conducting materials implemented in most cases as high
mobility electron transport layers in combination with an air-
stable metal cathode,
12–17
and the incorporation of ultra thin
layers based on ferroelectric insulators to amplify the local
electric eld and, thus, promote exciton dissociation and elec-
tron–hole separation.
9,18,19
Yet, the obtained V
oc
values remain
below their theoretical limits (i.e. the difference between the
E
HOMO
of the donor and the E
LUMO
of the acceptor).
8
On the other hand, planar organic molecules with unusual
electronic and optical properties, such as porphyrins and
phthalocyanines, have been intensively investigated due to their
unique structure, based on two-dimensional conjugated cores,
a
Department of Microelectronics, Institute of Advanced Materials, Physicochemical
Processes, Nanotechnology and Microsystems (IAMPPNM), National Center for
Scientic Research “Demokritos”, 153 10 Aghia Paraskevi Attikis, Athens, Greece.
E-mail: mariva@imel.demokritos.gr
b
Department of Physics, University of Patras, 26500 Patras, Greece
c
Department of Chemical Engineering, University of Patras, 26500 Patras, Greece
d
Laboratory of Bioinorganic Chemistry, Chemistry Department, University of Crete,
Voutes Campus, 71003 Heraklion, Crete, Greece
† Electronic supplementary information (ESI) available: Materials and methods,
ESI text, Fig. S1–S9. See DOI: 10.1039/c3ta13107f
Cite this: J. Mater. Chem. A, 2014, 2,
182
Received 7th August 2013
Accepted 17th October 2013
DOI: 10.1039/c3ta13107f
www.rsc.org/MaterialsA
182 | J. Mater. Chem. A, 2014, 2, 182–192 This journal is © The Royal Society of Chemistry 2014
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