7 research outputs found
Active Layer-Incorporated, Spectrally Tuned Au/SiO<sub>2</sub> Core/Shell Nanorod-Based Light Trapping for Organic Photovoltaics
We demonstrate that incorporation of octadecyltrimethoxysilane (OTMS)-functionalized, spectrally tuned, gold/silica (Au/SiO<sub>2</sub>) core/shell nanospheres and nanorods into the active layer of an organic photovoltaic (OPV) device led to an increase in photoconversion efficiency (PCE). A silica shell layer was added onto Au core nanospheres and nanorods in order to provide an electrically insulating surface that does not interfere with carrier generation and transport inside the active layer. Functionalization of the Au/SiO<sub>2</sub> core/shell nanoparticles with the OTMS organic ligand was then necessary to transfer the Au/SiO<sub>2</sub> core/shell nanoparticles from an ethanol solution into an OPV polymer-compatible solvent, such as dichlorobenzene. The OTMS-functionalized Au/SiO<sub>2</sub> core/shell nanorods and nanospheres were then incorporated into the active layers of two OPV polymer systems: a poly(3-hexylthiophene):[6,6]-phenyl-C61-butyric acid methyl ester (P3HT:PCB<sub>60</sub>M) OPV device and a poly[2,6-4,8-di(5-ethylhexylthienyl)benzo[1,2-<i>b</i>;3,4-<i>b</i>]dithiophene-<i>alt</i>-5-dibutyloctyl-3,6-bis(5-bromothiophen-2-yl)pyrrolo[3,4-<i>c</i>]pyrrole-1,4-dione] (PBDTT-DPP:PC<sub>60</sub>BM) OPV device. For the P3HT:PC<sub>60</sub>BM polymer with a band edge of ∼700 nm, the addition of the core/shell nanorods with an aspect ratio (AR) of ∼2.5 (extinction peak ∼670 nm) resulted in a 7.1% improvement in PCE, while for the PBDTT-DPP:PC<sub>60</sub>BM polymer with a band edge of ∼860 nm, the addition of core/shell nanorods with an AR of ∼4 (extinction peak ∼830 nm) resulted in a 14.4% improvement in PCE. The addition of Au/SiO<sub>2</sub> core/shell nanospheres to the P3HT:PC<sub>60</sub>BM polymer resulted in a 2.7% improvement in PCE, while their addition to a PBDTT-DPP:PC<sub>60</sub>BM polymer resulted in a 9.1% improvement. The PCE and <i>J</i><sub>sc</sub> enhancements were consistent with external quantum efficiency (EQE) measurements, and the EQE enhancements spectrally matched the extinction spectra of Au/SiO<sub>2</sub> nanospheres and nanorods in both OPV polymer systems
Interface Engineering of High-Performance Perovskite Photodetectors Based on PVP/SnO<sub>2</sub> Electron Transport Layer
Hybrid
organic–inorganic perovskites have attracted intensive interest
as active materials for high-performance photodetectors. However,
studies on the electron transport layer (ETL) and its influence on
the response time of photodetectors remain limited. Herein, we compare
the performances of perovskite photodetectors with TiO<sub>2</sub> and SnO<sub>2</sub> ETLs, especially on the response time. Both
photodetectors exhibit a high on/off current ratio of 10<sup>5</sup>, a large detectivity around 10<sup>12</sup> Jones, and a linear
dynamic range over 80 dB. The SnO<sub>2</sub>-based perovskite photodiodes
show ultrahigh response rates of 3 and 6 μs for the rise and
decay times, respectively. However, photodetectors with TiO<sub>2</sub> ETLs have low responsivity and long response time at low driving
voltage, which is attributed to the electron extraction barrier at
the TiO<sub>2</sub>/perovskite interface and the charge traps in the
TiO<sub>2</sub> layer. Furthermore, the dark current of SnO<sub>2</sub>-based perovskite photodiodes is effectively suppressed by inserting
a poly(vinylpyrrolidone) interlayer, and then the on/off current ratio
increases to 1.2 × 10<sup>6</sup>, corresponding to an improvement
of 1 order of magnitude. Such low-cost, solution-processable perovskite
photodetectors with high performance show promising potential for
future optoelectronic applications
Systematic Investigation of Benzodithiophene- and Diketopyrrolopyrrole-Based Low-Bandgap Polymers Designed for Single Junction and Tandem Polymer Solar Cells
The tandem solar cell architecture is an effective way
to harvest
a broader part of the solar spectrum and make better use of the photonic
energy than the single junction cell. Here, we present the design,
synthesis, and characterization of a series of new low bandgap polymers
specifically for tandem polymer solar cells. These polymers have a
backbone based on the benzodithiophene (BDT) and diketopyrrolopyrrole
(DPP) units. Alkylthienyl and alkylphenyl moieties were incorporated
onto the BDT unit to form BDTT and BDTP units, respectively; a furan
moiety was incorporated onto the DPP unit in place of thiophene to
form the FDPP unit. Low bandgap polymers (bandgap = 1.4–1.5
eV) were prepared using BDTT, BDTP, FDPP, and DPP units via Stille-coupling
polymerization. These structural modifications lead to polymers with
different optical, electrochemical, and electronic properties. Single
junction solar cells were fabricated, and the polymer:PC<sub>71</sub>BM active layer morphology was optimized by adding 1,8-diiodooctane
(DIO) as an additive. In the single-layer photovoltaic device, they
showed power conversion efficiencies (PCEs) of 3–6%. When the
polymers were applied in tandem solar cells, PCEs over 8% were reached,
demonstrating their great potential for high efficiency tandem polymer
solar cells
Selective Direct Growth of Atomic Layered HfS<sub>2</sub> on Hexagonal Boron Nitride for High Performance Photodetectors
Hafnium disulfide
(HfS<sub>2</sub>) has attracted significant interest
because of the predicted excellent electronic properties superior
to group VIB transition metal dichalcogenides. On the other hand,
atomically thin hexagonal boron nitride (h-BN) is an ideal dielectric
substrate for optoelectronic applications of other 2D materials. Here,
for the first time, we report the direct growth of high-quality atomic
layered HfS<sub>2</sub> on few-layer h-BN transferred on SiO<sub>2</sub>/Si substrates by chemical vapor deposition. It was found that the
HfS<sub>2</sub> layers are selectively grown on h-BN rather than on
SiO<sub>2</sub>/Si. Density functional theory calculations are performed
to help understand the mechanism of selective growth of HfS<sub>2</sub>. Furthermore, the photodetectors based on the HfS<sub>2</sub>/h-BN
heterostructures exhibit excellent visible-light sensing performance,
such as a high on/off ratio of more than 10<sup>5</sup>, an ultrafast
response rate of about 200 μs, a high responsivity of 26.5 mA
W<sup>–1</sup>, and a competitive detectivity exceeding 3 ×
10<sup>11</sup> Jones, superior to the vast majority of the reported
2D materials based photodetectors. The remarkable performance of the
HfS<sub>2</sub>/h-BN photodetector is attributed to the unique features
of 2D h-BN substrate
A Selenophene Containing Benzodithiophene-<i>alt</i>-thienothiophene Polymer for Additive-Free High Performance Solar Cell
A selenophene-modified
PTB7, PBDTSe-TT, is reported. The structure adjustment carried out
by alkylselenophene substitution on the BDT building block is shown
to slightly affect the polymer’s electronic property, and an
enlarged <i>V</i><sub>OC</sub> of the resulting photovoltaic
device is observed. More importantly, the PBDTSe-TT:PC<sub>71</sub>BM bulk-heterojunction thin film morphology can be optimized through
this modification. As a result, an efficient PCE of 8.8% is achieved
without using any solvent additive or special interfacial layer. In
addition, the PBDTSe-TT-based device is relatively stable under thermal
stress, making it a good candidate for fabricating stacking cells.
Finally, a ∼10% PCE tandem device is demonstrated by using
identical PBDTSe-TT:PC<sub>71</sub>BM subcells
Low-Temperature Solution-Processed Perovskite Solar Cells with High Efficiency and Flexibility
Perovskite compounds have attracted recently great attention in photovoltaic research. The devices are typically fabricated using condensed or mesoporous TiO<sub>2</sub> as the electron transport layer and 2,2′7,7′-tetrakis-(<i>N</i>,<i>N</i>-dip-methoxyphenylamine)9,9′-spirobifluorene as the hole transport layer. However, the high-temperature processing (450 °C) requirement of the TiO<sub>2</sub> layer could hinder the widespread adoption of the technology. In this report, we adopted a low-temperature processing technique to attain high-efficiency devices in both rigid and flexible substrates, using device structure substrate/ITO/PEDOT:PSS/CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3–<i>x</i></sub>Cl<sub><i>x</i></sub>/PCBM/Al, where PEDOT:PSS and PCBM are used as hole and electron transport layers, respectively. Mixed halide perovskite, CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3–<i>x</i></sub>Cl<sub><i>x</i></sub>, was used due to its long carrier lifetime and good electrical properties. All of these layers are solution-processed under 120 °C. Based on the proposed device structure, power conversion efficiency (PCE) of 11.5% is obtained in rigid substrates (glass/ITO), and a 9.2% PCE is achieved for a polyethylene terephthalate/ITO flexible substrate
Integrated Perovskite/Bulk-Heterojunction toward Efficient Solar Cells
We
successfully demonstrated an integrated perovskite/bulk-heterojunction
(BHJ) photovoltaic device for efficient light harvesting and energy
conversion. Our device efficiently integrated two photovoltaic layers,
namely a perovskite film and organic BHJ film, into the device. The
device structure is ITO/TiO<sub>2</sub>/perovskite/BHJ/MoO<sub>3</sub>/Ag. A wide bandgap small molecule DOR3T-TBDT was used as donor in
the BHJ film, and a power conversion efficiency (PCE) of 14.3% was
achieved in the integrated device with a high short circuit current
density (<i>J</i><sub>SC</sub>) of 21.2 mA cm<sup>–2</sup>. The higher <i>J</i><sub>SC</sub> as compared to that
of the traditional perovskite/HTL (hole transporting layer) device
(19.3 mA cm<sup>–2</sup>) indicates that the BHJ film absorbs
light and contributes to the current density of the device. Our result
further suggests that the HTL in traditional perovskite solar cell,
even with good light absorption capability, cannot contribute to the
overall device photocurrent, unless this HTL becomes a BHJ layer (by
adding electron transporting material like PC<sub>71</sub>BM)