Donor–p–donor type hole transporting materials:
marked p-bridge effects on optoelectronic
properties, solid-state structure, and perovskite
solar cell efficiency†
S. Paek,
a
I. Zimmermann,
a
P. Gao,
*
a
P. Gratia,
a
K. Rakstys,
a
G. Grancini,
a
Mohammad Khaja Nazeeruddin,
*
a
Malik Abdul Rub,
b
Samia A. Kosa,
b
Khalid A. Alamry
b
and Abdullah M. Asiri
b
Donor–p-bridge–donor type oligomers (D–p–D) have been studied intensively as active materials for
organic optoelectronic devices. In this study, we introduce three new D–p–D type organic
semiconductors incorporating thiophene or thienothiophene with two electron-rich TPA units, which
can be easily synthesized from commercially available materials. A thorough comparison of their
optoelectronic and structural properties was conducted, revealing the strong influence of the extent of
longitudinal p-bridge conjugation on both the solid structure of the organic semiconductive materials
and their photovoltaic performance when applied as hole transporting materials (HTM) in perovskite
solar cells. Single-crystal measurements and time-resolved photoluminescence (TRPL) studies indicate
that these coplanar donor–p–donor type HTMs could be promising alternatives to state-of-the-art
spiro-OMeTAD, due to the multiple intermolecular short contacts as charge transporting channels and
efficient charge extraction properties from the perovskite layer. The optimized devices with PEH-9
exhibited an impressive PCE of 16.9% under standard global AM 1.5 illumination with minimized
hysteretic behaviour, which is comparable to that of devices using spiro-OMeTAD under similar
conditions. Ambient stability after 400 h revealed that 93% of the energy conversion efficiency was
retained for PEH-9, indicating that the devices had good long-term stability.
Introduction
Organometal halide perovskite solar cells (PSCs) exhibiting
high power conversion efficiencies (PCEs) may provide inex-
pensive, renewable sources of solar electricity via low-cost
materials and fabrication techniques.
1–3
PCEs of PSCs have been
quickly increased from 3.8 to 22.1% as certied by the National
Renewable Energy Laboratory (NREL)
4
due to their intrinsic
advantages such as broad absorption in the visible region,
5
high
absorption coefficients,
6
high charge carrier mobility
7
and long
diffusion length.
8
In such devices, the photoactive layer nor-
mally consists of a pure/blended polycrystalline layer of perov-
skite semiconductor [APbX
3
,A ¼ MAI, FAI, Cs; X ¼ Cl, Br, I] that
is imbedded between a layer of electron transporting material
(ETM) and a hole transporting material (HTM).
2
An attractive
approach to push PSCs to industry and market, besides devel-
oping unconventional device structures
9
and more complicated
perovskite compositions,
10
is to explore new contact/interfacial
materials, particularly HTMs.
11
HTMs play an important role in
determining the photovoltaic performance and long-term
stability of the perovskite solar cells. Among the many HTMs
developed, 2,2
0
,7,7
0
-tetrakis(N,N-di-p-methoxyphenylamine)-
9,9
0
-spirobiuorene (spiro-OMeTAD) is by far the most studied
and used molecular p-type HTM with a recently reported PCE of
20.8%.
12
However, spiro-OMeTAD is very expensive owing to the
need for sublimation for purication. In this regard, the
development of cost-effective and efficient HTMs remains
a problem.
Recently, impressive photovoltaic performance has been
achieved using molecular HTMs, such as thiophene deriva-
tives,
13,14
3,4-ethylenedioxythiophene derivatives,
15–17
spiro-
OMeTAD derivatives,
18,19
truxene-based derivatives,
20
carbazole
derivatives,
21
etc.
22
Their characterization provides fundamental
information on how molecular modications affect PCE by
altering arylamine-substitution, p-system size, steric geometry,
and carrier mobility. However, the interesting question of how
a
Group for Molecular Engineering of Functional Materials, Ecole Polytechnique
Federale de Lausanne Valais Wallis, Rue de l'Indutrie 17, 1950 Sion, Valais,
Switzerland. E-mail: mdkhaja.nazeeruddin@ep.ch; peng.gao@ep.ch
b
Center of Excellence for Advanced Materials Research (CEAMR), King Abdulaziz,
University, Jeddah, Saudi Arabia
† Electronic supplementary information (ESI) available. CCDC 1446682–1446684.
For ESI and crystallographic data in CIF or other electronic format see DOI:
10.1039/c6sc01478j
Cite this: Chem. Sci., 2016, 7, 6068
Received 4th April 2016
Accepted 24th May 2016
DOI: 10.1039/c6sc01478j
www.rsc.org/chemicalscience
6068 | Chem. Sci., 2016, 7, 6068–6075 This journal is © The Royal Society of Chemistry 2016
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