P.M. Kuznetsov et al. / Tetrahedron Letters xxx (xxxx) xxx
3
Table 1
Physicochemical, optical, and electrochemical properties of polymers P1 and P2.
Eogpt, eV
Eooxnset,V vs. Fc+/Fc
HOMO, eV
LUMO, eVb
Td, °C
Tm/Tc, °C
a
sol
max
k
/kfmilamx/kefidlmge, nm
Mw, kDa
Mw/Mn
P1
P2
51
78
1.3
1.8
525/623/729
529/664/745
1.70
1.66
0.52
0.69
À5.62
À5.79
À3.92
À4.13
335
320
278/244
n/a
a
HOMO energy was estimated from onset of the oxidation potential using Fermi energy of À5.1 eV for the Fc+/Fc redox couple.
b
LUMO level was estimated as Eogpt + HOMO.
(60 nm)/Al (50 nm). The active fullerene derivative ([70]PCBM) –
conjugated polymer blend films were blade-coated in air from
1,2-dichlorobenzene as a standard solvent and from eco-friendly
m-xylene. It is well known that the morphology of active layer
films and consequently the photovoltaic performance of the OSCs
can be improved by using additives with high-boiling points [22].
Therefore, screening of different compounds revealed diphenyl
ether (DPE) as a promising processing additive for P1(P2)/[70]
PCBM blends.
On the other hand, enhancing the performance of OSCs as well
as their stability is closely related to interface engineering [23,24].
Therefore, we inserted polyhydroquinone [25] (PHQ) or fullerene
derivative BLF-P [26] as interfacial buffer layers between the active
layer and top electrode (Fig. 2b). These compounds were selected
because their LUMO energy levels match the LUMO of the acceptor
component [70]PCBM and the work function of the metal
electrodes.
The parameters of devices fabricated under different conditions
tested during optimization are shown in Table S1 (ESI). The photo-
voltaic characteristics of optimized solar cells are presented in
Table 2. Current density–voltage (J-V) curves and external quan-
tum efficiency spectra (EQE) measured under simulated AM1.5G
illumination (100 mW cmÀ2) are shown in Fig. 3. Small-area OSCs
based on polymer P1 showed efficiencies of ~7%. When using
dichlorobenzene as a solvent, the best performance was achieved
by adding 1% of DPE and introducing a PHQ buffer layer, while
xylene-processed OSCs showed the best characteristics without
using any interfacial layers (Table S1, ESI). Both devices demon-
strated high and comparable short-circuit current densities (JSC),
which match well with photocurrents obtained by integration of
the corresponding EQE spectra.
As illustrated in Fig. 3 and Table 2, benzoxadiazole-containing
polymer P2 showed lower efficiencies in solar cells: 6.4% and
5.7% when processed from dichlorobenzene and xylene, respec-
tively. Solar cells exhibited lower JSC values and fill factors (FF)
compared to that of P1-based devices that might be originating
from poor charge transport or inappropriate morphology of the
composite active layer [27]. Notably, OSCs with polymer P2 dis-
played significantly enhanced VOC that is in accordance with the
low-lying HOMO energy of this donor polymer. It is worth noting
that PHQ or BLF-P buffer layers did not improve the performance
of P2-based solar cells (Table S1, ESI).
Fig. 1. Absorption spectra (a) and cyclic voltammograms of conjugated polymers
P1 and P2 (b).
ox
levels of the polymers were calculated from E
potentials and
onset
using the value of À5.1 eV as the potential of the Fc+/Fc redox couple
in the Fermi energy scale [17]. Conjugated polymer P2 comprising
benzoxadiazole acceptor blocks showed 0.17 eV lower HOMO energy
compared to that of benzothiadiazole-containing P1. The observed
effect can be related to the higher electronegativity of the oxygen
atom [18,19]. Considering this fact, higher open-circuit voltages
can be obtained for solar cells based on P2 [20]. The LUMO energies
were calculated based on HOMO energies and the optical bandgap of
P1 and P2.
We investigated charge career mobilities for optimized poly-
mer-fullerene blends using the space-charge limited current
(SCLC) method [28]. The measurements were performed for the
hole-only
(ITO/PEDOT:PSS(60
nm)/blend/MoO3(22
nm)/Ag
(120 nm) and the electron-only (ITO/Yb(15 nm)/blend/Ca) devices.
It was found that the optimized P1/[70]PCBM blends have higher
and more balanced hole (lh) and electron (le) mobilities than
P2/[70]PCBM blends (Table 2). Thus, a more efficient charge trans-
port in P1-based films can explain the higher JSC and FF values
achieved for devices.
In order to understand the morphology of P1/[70]PCBM and P2/
[70]PCBM blend films processed from DCB and m-xylene, atomic
force microscopy (AFM) measurements were performed. AFM
topography height images are shown in Fig. 4 and Figs. S11 and
S12 (ESI).
Fig. 2 shows the energy levels diagram of the photovoltaic
device components. The difference between HOMO and LUMO
levels of the polymers and [70]PCBM ([6,6]-phenyl-C71-butyric
acid methyl ester) are greater than 0.3 eV, which is beneficial for
exciton dissociation into free charge carriers [21].
We used standard bulk heterojunction organic solar cell config-
uration ITO/PEDOT:PSS (60 nm)/active layer (100–200 nm)/Mg
Please cite this article as: P. M. Kuznetsov, S. L. Nikitenko, I. E. Kuznetsov et al., Thiazolothiazole-based conjugated polymers for blade-coated organic solar