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2013 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim 2993
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Jesse R. Manders, Sai-Wing Tsang, Michael J. Hartel, Tzung-Han Lai, Song Chen,
Chad M. Amb,* John R. Reynolds,* and Franky So*
Solution-Processed Nickel Oxide Hole Transport Layers in
High Efficiency Polymer Photovoltaic Cells
1. Introduction
In a society concerned with environ-
mental, economic, and geopolitical con-
sequences of energy consumption, new
alternatives to traditional energy sources
are needed. With rapid progress being
made in organic photovoltaics, they are
becoming a viable source of renewable
energy, as power conversion efficiencies
(PCEs) exceeding 8% have been demon-
strated.
[1,2]
Traditional bulk heterojunction
polymer solar cells consist of a transparent
indium tin oxide (ITO) anode, a hole trans-
port layer, a photoactive layer, and a top
cathode. Hole transport layers must have
high optical transparency, good chemical
stability, a large ionization potential, and
good electron blocking capability.
In a typical polymer solar cell, poly(3,4-
ethylenedioxythiophene):poly(styrenes
ulfonate) (PEDOT:PSS) is used as the
hole-transporting layer (HTL) and has
a work function ( Φ) of 5.2 eV. However,
its acidity, tendency to absorb water, and
inability to block electrons effectively are
factors which contribute to device per-
formance problems and degradation.
[3]
Nickel oxide is emerging as an alternative
HTL for polymer solar cells.
[4–14]
Pure, stoichiometric NiO is an
excellent insulator, with room temperature conductivity on the
order of 10
−13
S cm
−1
,
[15]
while non-stoichiometric NiO is a wide
bandgap p-type semiconductor.
[16–21]
The p-type conductivity of
NiO originates from two positively charged holes which accom-
pany each Ni
2 +
vacancy in the lattice for charge neutrality.
[16,22,23]
These holes are quasi-localized on Ni
2 +
ions near the vacancy in
the lattice, generating two Ni
3 +
ions for each Ni
2 +
vacancy.
[16,24]
The valence band edge of NiO is well-aligned to the highest
occupied molecular orbital (HOMO) levels of many p-type con-
jugated polymers for photovoltaics.
[12,21]
Irwin et al. first demonstrated an enhancement in polymer
solar cell performance with a NiO electron blocking layer depos-
ited via pulsed laser deposition.
[12,25]
Recently, solution-proc-
essed NiO was also reported for polymer photovoltaics.
[13,14,21]
A
nickel ink made from nickel formate and ethylenediamine was
used as the precursor in those reports. Here, we chose nickel
acetate tetrahydrate and monoethanolamine precursors in an
ethanolic solution, as this presents a set of materials not yet
The detailed characterization of solution-derived nickel (II) oxide (NiO) hole-
transporting layer (HTL) films and their application in high efficiency organic
photovoltaic (OPV) cells is reported. The NiO precursor solution is examined
in situ to determine the chemical species present. Coordination complexes of
monoethanolamine (MEA) with Ni in ethanol thermally decompose to form
non-stoichiometric NiO. Specifically, the [Ni(MEA)
2
(OAc)]
+
ion is found to
be the most prevalent species in the precursor solution. The defect-induced
Ni
3 +
ion, which is present in non-stoichiometric NiO and signifies the p-type
conduction of NiO, as well as the dipolar nickel oxyhydroxide (NiOOH)
species are confirmed using X-ray photoelectron spectroscopy. Bulk hetero-
junction (BHJ) solar cells with a polymer/fullerene photoactive layer blend
composed of poly-dithienogermole-thienopyrrolodione (pDTG-TPD) and
[6,6]-phenyl-C71-butyric acid methyl ester (PC
71
BM) are fabricated using
these solution-processed NiO films. The resulting devices show an average
power conversion efficiency (PCE) of 7.8%, which is a 15% improvement over
devices utilizing a poly(3,4-ethylenedioxythiophene):poly(styrenesulfonate)
(PEDOT:PSS) HTL. The enhancement is due to the optical resonance in the
solar cell and the hydrophobicity of NiO, which promotes a more homoge-
neous donor/acceptor morphology in the active layer at the NiO/BHJ inter-
face. Finally, devices incorporating NiO as a HTL are more stable in air than
devices using PEDOT:PSS.
J. R. Manders, Dr. S.-W. Tsang, M. J. Hartel, T.-H. Lai,
S. Chen, Prof. F. So
Department of Materials Science and Engineering
University of Florida
Gainesville, FL 32611 USA
E-mail: fso@mse.ufl.edu
Dr. C. M. Amb
The George and Josephine Butler Polymer Research Laboratory
Department of Chemistry
Center for Macromolecular Science and Engineering
University of Florida
Gainesville, FL 32611 USA
E-mail: chad.amb@hotmail.com
Prof. J. R. Reynolds
School of Chemistry and Biochemistry
School of Materials Science and Engineering
Center for Organic Photonics and Electronics
Georgia Institute of Technology
Atlanta, GA 30332-0400 USA
E-mail:r eynolds@chemistry.gatech.edu
DOI:10. 1002/adfm.201202269
Adv. Funct. Mater. 2013, 23, 2993–3001