31 research outputs found
Additional file 1 of MiRKAT-S: a community-level test of association between the microbiota and survival times
PDF file includes supplemental tables (Tables S1âS3) and figures (Figures S1âS2). (PDF 933 kb
Composition-Dependent Light-Induced Dipole Moment Change in Organometal Halide Perovskites
In
this work we investigate the compositional dependence of electric
dipole moment in AMX<sub>3</sub> (A: organic; M: metal; X: halogen)
perovskite structures using modulation electroabsorption (EA) spectroscopy.
By sampling various device structures, we show that the second harmonic
EA spectra reflect the intrinsic dipolar property of perovskite films
in a layered configuration. A quantitative analysis of the EA spectra
of CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub>, NH<sub>2</sub>CHNH<sub>2</sub>PbI<sub>3</sub>, and CH<sub>3</sub>NH<sub>3</sub>Sn<sub>0.4</sub>Pb<sub>0.6</sub>I<sub>3</sub> is provided to compare the impact of
the organic and metal cations on the photoinduced response of dipole
moment. Based on the EA results, we propose that the A and M cations
could both largely affect the dielectric and dipolar properties of
the perovskite materials, but through different mechanisms, such as
ionic polarization, rotation of molecular dipoles and charge migration.
These processes occur at different time scales and thus result in
a frequency-dependent dipole response
Carrier-Activated Polarization in Organometal Halide Perovskites
Organometal
halide perovskite solar cells exhibit a strong polarization
effect under light illumination. This unique property, although widely
observed, has not been well understood. In this work, we carried out
a systematic investigation on this phenomenon by varying the perovskite
composition and device configurations. We find that the light-enhanced
strong polarization is a general phenomenon that occurs in all tested
perovskite materials. The organic molecular dipoles affect the polarization
at high frequency range, while the photoexcited free carriers and
the interface between perovskite and its neighboring layers dominate
the low-frequency response. In particular, our study suggests that
the giant low-frequency capacitance enhancement originates from native
defects and their accompanying defect dipoles, which need to be activated
by photogenerated charge carriers. The high flexibility of the perovskite
lattice facilitates the formation of these defects, and the dipole
effect is enhanced at the interface regions where an electric double-layer
capacitor is formed. This work sheds light on the understanding of
the light-induced polarization mechanisms of perovskite materials
In Situ Probing of the Charge Transport Process at the Polymer/Fullerene Heterojunction Interface
The polymer/fullerene interface (PFI)
in polymer solar cells (PSCs)
provides an energetic offset for exciton dissociation while at the
same time influencing local transport of photocarriers adjacent to
the interface. In this paper, we introduce a heterojunction field-effect
transistor (FET) structure in charge modulation spectroscopy (CMS)
to enable in situ probing of the charge transport process at PFIs.
The PFIs formed by fullerene/crystalline polymer and fullerene/amorphous
polymer systems are studied and compared, respectively. By correlating
the steady-state and frequency-dependent CMS responses of pure polymer,
polymer/fullerene bilayer, and polymer/fullerene blend FETs, we demonstrate
that through different charge localization effects the interface fullerene
molecules can influence the hole transport in both crystalline and
amorphous polymer phases. We propose a trade-off between charge transfer
and charge transport at PFIs with an aim to enhance the engineering
of molecular orientation and packing at the donor–acceptor
interface for high-performance PSCs
Photocurrent Enhancement of HgTe Quantum Dot Photodiodes by Plasmonic Gold Nanorod Structures
The near-field effects of noble metal nanoparticles can be utilized to enhance the performance of inorganic/organic photosensing devices, such as solar cells and photodetectors. In this work, we developed a well-controlled fabrication strategy to incorporate Au nanostructures into HgTe quantum dot (QD)/ZnO heterojunction photodiode photodetectors. Through an electrostatic immobilization and dry transfer protocol, a layer of Au nanorods with uniform distribution and controllable density is embedded at different depths in the ZnO layer for systematic comparison. More than 80 and 240% increments of average short-circuit current density (<i>J</i><sub>sc</sub>) are observed in the devices with Au nanorods covered by ∼7.5 and ∼4.5 nm ZnO layers, respectively. A periodic finite-difference time-domain (FDTD) simulation model is developed to analyze the depth-dependent property and confirm the mechanism of plasmon-enhanced light absorption in the QD layer. The wavelength-dependent external quantum efficiency spectra suggest that the exciton dissociation and charge extraction efficiencies are also enhanced by the Au nanorods, likely due to local electric field effects. The photodetection performance of the photodiodes is characterized, and the results show that the plasmonic structure improves the overall infrared detectivity of the HgTe QD photodetectors without affecting their temporal response. Our fabrication strategy and theoretical and experimental findings provide useful insight into the applications of metal nanostructures to enhance the performance of organic/inorganic hybrid optoelectronic devices
Spectroscopic Study of Charge Transport at Organic Solid–Water Interface
Charge
transport in an organic solid and its coupling with the
neighboring aqueous biological environment dictates the performance
of many organic bioelectronic devices. Understanding how the transport
property at the solid–water interface is influenced by the
surface structure characteristics of the organic solid is essential
for rational design of organic bioelectronics and chemical sensors.
However, <i>in situ</i> probing such structure–property
relationships has been difficult due to lack of experimental techniques
with sufficient sensitivity to the water-buried interface. Here, we
demonstrate a charge accumulation spectroscopy (CAS)-based protocol,
exploiting water-gated organic field-effect transistor as the testing
platform, to investigate the structure-dependent localization of polaronic
charge carriers at the organic semiconductor–liquid interface.
Our results reveal that the degree of charge delocalization is reduced
drastically when the charge carriers are moved from the bulk semiconductor
to the semiconductor–water interface, suggesting the existence
of a highly disordered surface layer in contact with water. It is
also found that the charge delocalization could be further reduced
by intercalation of chloride ions (from salt water) in the semiconductor
surface layer. This study suggests that the spectroscopic signatures
of polaronic charge carriers could be a sensitive probe to detect
the structure-dependent charge localization at organic solid–liquid
interfaces
Flexible Piezoelectric-Induced Pressure Sensors for Static Measurements Based on Nanowires/Graphene Heterostructures
The
piezoelectric effect is widely applied in pressure sensors
for the detection of dynamic signals. However, these piezoelectric-induced
pressure sensors have challenges in measuring static signals that
are based on the transient flow of electrons in an external load as
driven by the piezopotential arisen from dynamic stress. Here, we
present a pressure sensor with nanowires/graphene heterostructures
for static measurements based on the synergistic mechanisms between
strain-induced polarization charges in piezoelectric nanowires and
the caused change of carrier scattering in graphene. Compared to the
conventional piezoelectric nanowire or graphene pressure sensors,
this sensor is capable of measuring static pressures with a sensitivity
of up to 9.4 × 10<sup>–3</sup> kPa<sup>–1</sup> and a fast response time down to 5–7 ms. This demonstration
of pressure sensors shows great potential in the applications of electronic
skin and wearable devices
Energy Level Modification in Lead Sulfide Quantum Dot Thin Films through Ligand Exchange
The electronic properties of colloidal quantum dots (QDs) are critically dependent on both QD size and surface chemistry. Modification of quantum confinement provides control of the QD bandgap, while ligand-induced surface dipoles present a hitherto underutilized means of control over the absolute energy levels of QDs within electronic devices. Here, we show that the energy levels of lead sulfide QDs, measured by ultraviolet photoelectron spectroscopy, shift by up to 0.9 eV between different chemical ligand treatments. The directions of these energy shifts match the results of atomistic density functional theory simulations and scale with the ligand dipole moment. Trends in the performance of photovoltaic devices employing ligand-modified QD films are consistent with the measured energy level shifts. These results identify surface-chemistry-mediated energy level shifts as a means of predictably controlling the electronic properties of colloidal QD films and as a versatile adjustable parameter in the performance optimization of QD optoelectronic devices
Solution-Processed Ambipolar Organic Thin-Film Transistors by Blending p- and n‑Type Semiconductors: Solid Solution versus Microphase Separation
Here,
we report solid solution of p- and n-type organic semiconductors as
a new type of p–n blend for solution-processed ambipolar organic
thin film transistors (OTFTs). This study compares the solid-solution
films of silylethynylated tetraazapentacene <b>1</b> (acceptor)
and silylethynylated pentacene <b>2</b> (donor) with the microphase-separated
films of <b>1</b> and <b>3</b>, a heptagon-embedded analogue
of <b>2</b>. It is found that the solid solutions of (<b>1</b>)<sub><i>x</i></sub>(<b>2</b>)<sub>1–<i>x</i></sub> function as ambipolar semiconductors, whose hole
and electron mobilities are tunable by varying the ratio of <b>1</b> and <b>2</b> in the solid solution. The OTFTs of (<b>1</b>)<sub>0.5</sub>(<b>2</b>)<sub>0.5</sub> exhibit relatively
balanced hole and electron mobilities comparable to the highest values
as reported for ambipolar OTFTs of stoichiometric donor–acceptor
cocrystals and microphase-separated p-n bulk heterojunctions. The
solid solution of (<b>1</b>)<sub>0.5</sub>(<b>2</b>)<sub>0.5</sub> and the microphase-separated blend of <b>1:3</b> (0.5:0.5)
in OTFTs exhibit different responses to light in terms of absorption
and photoeffect of OTFTs because the donor and acceptor are mixed
at molecular level with π–π stacking in the solid
solution
Ternary Bulk Heterojunction Photovoltaic Cells Composed of Small Molecule Donor Additive as Cascade Material
To explore the potential of ternary
blend bulk heterojunction (BHJ)
solar cells as a general platform for improving the performance of
organic photovoltaics, we studied a ternary BHJ system based on poly(3-hexylthiophene)
(P3HT), [6,6]-phenyl C61 butyric acid methyl ester (PC<sub>61</sub>BM), and DTDCTB. The optimized ternary structure containing a weight
ratio of 20% DTDCTB as the cascade material demonstrates a ∼25%
improvement of the power conversion efficiency (PCE) as compared to
the binary P3HT/PC<sub>61</sub>BM solar cells. A systematic spectroscopic
study is carried out to elucidate the underlying mechanism of charge
transfer in the ternary system. Wavelength-dependent external quantum
efficiency measurement confirms the contribution of DTDCTB to the
enhanced photocurrent. Photoinduced absorption spectroscopy and transient
photovoltage measurement reveal unambiguously that charges generated
in DTDCTB are efficiently transferred to and subsequently transported
in P3HT and PC<sub>61</sub>BM. The results also suggest that despite
the realization of cascade charge transfer, the bimolecular charge
recombination process in the ternary system is still dominated by
the P3HT/PC<sub>61</sub>BM interface