3 research outputs found
Packing Principles for Donor–Acceptor Oligomers from Analysis of Single Crystals
D–A conjugated
molecules are complicated in both their molecular
and their packing structures. In this perspective, we summarize more
than 40 crystal lattices of conjugated oligomers to identify the morphological
influence of each building block on the D–A molecules. These
lattice structures reveal not only the packing preferences of the
conjugated oligomers but also the conformational disorder in the lattices.
The presence of this disorder in slowly grown crystals implies that
attaining total long-range conformational order is challenging for
D–A oligomers, which are structurally complicated and readily
distorted and which have building blocks of incommensurate packing
dimensions. In optoelectronic applications, a decreased duration of
processing can prevent ordering and trap the thin films of D–A
oligomers from becoming crystalline phases. Although D–A oligomers
conform to packing principles in the formation of a single crystal,
their phase behaviors in the formation of active thin films are much
more difficult to comprehend. Continuous advances in methods of characterization
are still strongly required for the steps of attaining a true structure–property
relation of D–A oligomers in active films for optoelectronic
applications
Stepwise Structural Evolution of a DTS‑F<sub>2</sub>BT Oligomer and Influence of Structural Disorder on Organic Field Effect Transistors and Organic Photovoltaic Performance
An A–D–A oligomer,
DTSÂ(F<sub>2</sub>BT)<sub>2</sub>, was synthesized; its structural
evolution was studied with DSC,
POM, 2D-WAXD, and in-situ GI-XRD. The structural evolution of DTSÂ(F<sub>2</sub>BT)<sub>2</sub> is stepwise and kinetically slow. Both rapid
drying and the presence of PC<sub>71</sub>BM trapped DTSÂ(F<sub>2</sub>BT)<sub>2</sub> in a less ordered nematic (N) phase. PDMS-assisted
crystallization enabled a pristine DTSÂ(F<sub>2</sub>BT)<sub>2</sub> thin film to attain a more ordered equilibrium phase, and enhanced
the OFET mobility of DTSÂ(F<sub>2</sub>BT)<sub>2</sub>. In OPV devices,
DIO additive drove the DTSÂ(F<sub>2</sub>BT)<sub>2</sub> domains in
the DTSÂ(F<sub>2</sub>BT)<sub>2</sub>:PC<sub>71</sub>BM blended film
from the N phase toward the equilibrium phase, and resulted in enhanced
OPV performances. These results reveal the slow ordering process of
the A–D–A oligomer, and the importance of monitoring
the degree of structural evolution of the active thin films in organic
optoelectronics
Role of Tin Chloride in Tin-Rich Mixed-Halide Perovskites Applied as Mesoscopic Solar Cells with a Carbon Counter Electrode
We
report the synthesis and characterization of alloyed Sn–Pb
methylammonium mixed-halide perovskites (CH<sub>3</sub>NH<sub>3</sub>Sn<sub><i>y</i></sub>Pb<sub>1–<i>y</i></sub>I<sub>3–<i>x</i></sub>Cl<sub><i>x</i></sub>) to extend light harvesting toward the near-infrared region
for carbon-based mesoscopic solar cells free of organic hole-transport
layers. The proportions of Sn in perovskites are well-controlled by
mixing tin chloride (SnCl<sub>2</sub>) and lead iodide (PbI<sub>2</sub>) in varied stoichiometric ratios (<i>y</i> = 0–1).
SnCl<sub>2</sub> plays a key role in modifying the lattice structure
of the perovskite, showing anomalous optical and optoelectronic properties;
upon increasing the concentration of SnCl<sub>2</sub>, the variation
of the band gap and band energy differed from those of the SnI<sub>2</sub> precursor. The CH<sub>3</sub>NH<sub>3</sub>Sn<sub><i>y</i></sub>Pb<sub>1–<i>y</i></sub>I<sub>3–<i>x</i></sub>Cl<sub><i>x</i></sub> devices showed enhanced
photovoltaic performance upon increasing the proportion of SnCl<sub>2</sub> until <i>y</i> = 0.75, consistent with the corresponding
potential energy levels. The photovoltaic performance was further
improved upon adding 30 mol % tin fluoride (SnF<sub>2</sub>) with
device configuration FTO/TiO<sub>2</sub>/Al<sub>2</sub>O<sub>3</sub>/NiO/C, producing the best power conversion efficiency, 5.13%, with
great reproducibility and intrinsic stability