5 research outputs found
Decreased Charge Transport Barrier and Recombination of Organic Solar Cells by Constructing Interfacial Nanojunction with Annealing-Free ZnO and Al Layers
To
overcome drawbacks of the electron transport layer, such as
complex surface defects and unmatched energy levels, we successfully
employed a smart semiconductor–metal interfacial nanojunciton
in organic solar cells by evaporating an ultrathin Al interlayer onto
annealing-free ZnO electron transport layer, resulting in a high fill
factor of 73.68% and power conversion efficiency of 9.81%. The construction
of ZnO-Al nanojunction could effectively fill the surface defects
of ZnO and reduce its work function because of the electron transfer
from Al to ZnO by Fermi level equilibrium. The filling of surface
defects decreased the interfacial carrier recombination in midgap
trap states. The reduced surface work function of ZnO-Al remodulated
the interfacial characteristics between ZnO and [6,6]-phenyl C71-butyric
acid methyl ester (PC<sub>71</sub>BM), decreasing or even eliminating
the interfacial barrier against the electron transport, which is beneficial
to improve the electron extraction capacity. The filled surface defects
and reduced interfacial barrier were realistically observed by photoluminescence
measurements of ZnO film and the performance of electron injection
devices, respectively. This work provides a simple and effective method
to simultaneously solve the problems of surface defects and unmatched
energy level for the annealing-free ZnO or other metal oxide semiconductors,
paving a way for the future popularization in photovoltaic devices
Mechanism of Polyfluorene Interlayer in Ultraviolet Photodetector: Barrier-Blocking Electron Transport and Light-Inducing Hole Injection
A remarkable
performance ultraviolet (UV) photodetector was demonstrated
by introducing a polyÂ(9,9-dihexylfluorene) (PDHF) interlayer with
the roles of barrier-blocking electron transport and light-inducing
hole injection, leading to enhanced properties of the device both
in dark and under UV illumination. The PDHF interlayer can efficiently
block the electrons, which provides low dark current as well as the
reduced noise for devices. Furthermore, the accumulation of photogenerated
electrons causes the energy-band bending, leading to promoted gain
of holes under UV illumination. The specific detectivity of the device
with the PDHF interlayer reaches 1.86 × 10<sup>13</sup> cm Hz<sup>1/2</sup> W<sup>–1</sup>. Moreover, the response and recovery
speed have been upgraded due to the improvement of the carrier transport
mechanism
Boosted Electron Transport and Enlarged Built-In Potential by Eliminating the Interface Barrier in Organic Solar Cells
A smart interface
modification strategy was employed to simultaneously
improve short-circuit current density (<i>J</i><sub>sc</sub>) and open-circuit voltage (<i>V</i><sub>oc</sub>) by incorporating
a polyÂ[(9,9-bisÂ(3′-(<i>N</i>,<i>N</i>-dimethylamion)Âpropyl)-2,7-fluorene)-<i>alt</i>-2,7-(9,9-dioctyl)-fluorene] (PFN) interlayer between
a TiO<sub>2</sub> film and an active layer, arising from the fact
that PFN effectively eliminated the interface barrier between TiO<sub>2</sub> and the fullerene acceptor. The work function (WF) of TiO<sub>2</sub> was apparently reduced, which facilitated effective electron
transfer from the active layer to the TiO<sub>2</sub> electron transport
layer (ETL) and suppressed charge carrier recombination between contact
interfaces. Electron injection devices with and without a PFN interlayer
were fabricated to prove the eliminated electron barrier, meanwhile
photoluminescence (PL) and time-resolved transient photoluminescence
(TRTPL) were measured to probe much easier electron transfer from
[6,6]-phenyl C71-butyric acid methyl ester (PC<sub>71</sub>BM) acceptor
to TiO<sub>2</sub> ETL, contributing to enhanced <i>J</i><sub>sc</sub>. The shift in vacuum level altered the WF of PC<sub>71</sub>BM, which enlarged the internal electrical field at the donor/acceptor
interface and built-in potential (<i>V</i><sub>bi</sub>)
across the device. Dark current characteristics and Mott–Schottky
measurements indicated the enhancement of <i>V</i><sub>bi</sub>, benefiting to increased <i>V</i><sub>oc</sub>. Consequently,
the champion power conversion efficiency for a device with a PFN interlayer
of 0.50 mg/mL reached to 7.14%, which is much higher than the PCE
of 5.76% for the control device
Gas Sensors Based on Metal Sulfide Zn<sub>1–<i>x</i></sub>Cd<sub><i>x</i></sub>S Nanowires with Excellent Performance
Metal sulfide Zn<sub>1–<i>x</i></sub>Cd<sub><i>x</i></sub>S nanowires (NWs)
covering the entire compositional
range prepared by one step solvothermal method were used to fabricate
gas sensors. This is the first time for ternary metal sulfide nanostructures
to be used in the field of gas sensing. Surprisingly, the sensors
based on Zn<sub>1–<i>x</i></sub>Cd<sub><i>x</i></sub>S nanowires were found to exhibit enhanced response to ethanol
compared to those of binary CdS and ZnS NWs. Especially for the sensor
based on the Zn<sub>1–<i>x</i></sub>Cd<sub><i>x</i></sub>S (x = 0.4) NWs, a large sensor response (<i>s</i> = 12.8) and a quick rise time (2 s) and recovery time
(1 s) were observed at 206 °C toward 20 ppm ethanol, showing
preferred selectivity. A dynamic equilibrium mechanism of oxygen molecules
absorption process and carrier intensity change in the NWs was used
to explain the higher response of Zn<sub>1–<i>x</i></sub>Cd<sub><i>x</i></sub>S. The reason for the much quicker
response and recovery speed of the Zn<sub>1–<i>x</i></sub>Cd<sub><i>x</i></sub>S NWs than those of the binary
ZnS NWs was also discussed. These results demonstrated that the growth
of metal sulfide Zn<sub>1–<i>x</i></sub>Cd<sub><i>x</i></sub>S nanostructures can be utilized to develop gas sensors
with high performance
Self-Stabilized Quasi-2D Perovskite with an Ion-Migration-Inhibition Ligand for Pure Green LEDs
Perovskite light-emitting diodes (PeLEDs) have recently
achieved
a great breakthrough in external quantum efficiency (EQE). However,
the operational stability of pure primary color PeLEDs lags far behind
because of serious ion migration. Herein, a self-stabilized quasi-2D
perovskite is constructed with a strategically synthesized ion-migration-inhibition
ligand (IMIligand) to realize highly stable and efficient
pure green PeLEDs approaching the standard green light of Rec. 2020.
The IMIligand takes the role to not only eliminate migration
pathways and anchor halide ions to suppress the ion migration but
to also further enhance the crystalline orientation and energy transfer
in quasi-2D perovskites. Meanwhile, the self-stabilized quasi-2D perovskite
overcomes the degradation of electrical performance caused by conventional
exogenous passivation additives. Ultimately, the figure of merit of
the pure green quasi-2D PeLEDs is at least double that of previous
works. The devices achieve an EQE of 26.2% and operational stability
of 920 min at initial luminance of 1000 cd m–2