Different approaches to improving photoelectrochemical performance through α-Fe2O3 heterostructure design.

These are not the final page numbers! Ü Ü uniform. The low absorption/emission intensity of PNC supernatant is attributed to the low concentration of PNCs. This indicates that the as-formed PNCs can be easily collected by centrifugation (Supporting Information, Figure S5 b), which is desirable for cleaning and postprocessing in various applications.To explain the different capping effects of OA and APTES, we propose the following mechanism based on a dissolution-precipitation model (Figure 4 c). The dissolved precursors precipitate as PNCs at the DMF-toluene interface when the DMF precursor solution is injected into toluene. With OA as the capping ligand, the OA molecules adsorbed on the surface of the formed PNCs and PNSs diffuse from DMF to toluene, along with the products. However, the chain configuration of OA molecules cannot effectively prevent the products from dissolving back into DMF across the DMFtoluene interface and some OA ligands remain in the toluene phase because of their non-polar nature. The loss of OA ligands will result in a lack of ligands in the DMF phase, leading to the formation of large particles in the next round of precipitation. This effect becomes more pronounced when the concentrations of the precursors is high. On the contrary, the strong steric hindrance of APTES and the formation of silica can prohibit the dissolution of the as-formed PNCs back into DMF, which helps to maintain the original structural and optical properties of PNCs. Nevertheless, the PNC APTES-20 sample began to flocculate after standing for a few minutes (Supporting Information, Figure S7) because of hydrolysis of Si-O-C 2 H 5 groups attached to the PNC APTES surface, which generate hydroxy (-OH) groups (as indicated by FTIR spectra), resulting in a change in polarity and hydrogen bonding of the ligands.Water-induced degradation is a major problem for organic metal halide perovskites because protons are captured by methylammonium.[8] Similarly, they are also unstable towards other protic solvents such as alcohols.We hypothesized that PNC APTES may exhibit better stability because of the strong steric hindrance and hydrolysis properties of APTES, which reduces the access of protic solvent molecules to the PNCs surface. To test the stability of PNC APTES in protic solvents, 0.5 mg mL À1 of PNC precipitate capped by different ligands was dispersed in ethanol (Supporting Information, Figure S9 a and b). No emission was observed by the naked eye for PNC OA and PNC OABr dispersed in ethanol, and all XRD peaks (Supporting Information, Figure S9 c) of the decomposed products belong to rhombic PbBr 2 (JCPDS#31-0679). However, the PNC APTES precipitate showed high fluorescence intensity after sonication in ethanol, indicating better stability of PNC APTES in protic solvents.Long term stability tests were also conducted in different protic and polar solvents. As shown in Figure 5 a, the relative PL intensity of the PNC APTES-16 precipitate in isopropanol remained almost 70 % after 2.5 h. However, PNC precipitate showed p...

Long-chain saturated hydrocarbons and alkoxysilanes are ligands that are commonly used to passivate perovskite quantum dots (PQDs) to enhance their stability and optical properties. However, the insulating nature of these capping ligands creates an electronic energy barrier and impedes interparticle electronic coupling, thereby limiting device applications. One strategy to solve this problem is the use of short conductive aromatic ligands that allow delocalization of the electronic wave function from the PQDs, which, in turn, facilitates charge transport between PQDs by lowering the energy barrier. This is demonstrated with methylammonium lead bromide (MAPbBr 3 ) QDs prepared using benzylamine (BZA) and benzoic acid (BA) capping ligands. Optimized BZA-BA-MAPbBr 3 QDs are highly stable and show very high photoluminescence (PL) quantum yield (QY) (86%). More importantly, the BZA-BA-MAPbBr 3 QD film exhibits higher conductivity and carrier lifetime and more efficient charge extraction compared to PQDs with insulating ligands, as indicated by electrochemical measurements and transient photocurrent and photovoltage spectroscopy.

Organolead bromide CH3NH3PbBr3 perovskite nanocrystals (PNCs) with green photoluminescence (PL) have been synthesized using two different aliphatic ammonium capping ligands, octylammonium bromide (OABr) and octadecylammonium bromide (ODABr), resulting in PNC–OABr and PNC–ODABr, respectively. Structural studies by X-ray diffraction (XRD) and transmission electron microscopy (TEM) determined that the PNCs exhibit cubic phase crystal structure with average particle size dependent on capping ligand (3.9 ± 1.0 nm for PNC–OABr and 6.5 ± 1.4 nm for PNC–ODABr). The exciton dynamics of PNCs were investigated using femtosecond transient absorption (TA) techniques and singular value decomposition global fitting (SVD-GF), which revealed nonradiative recombination on the picosecond time scale mediated by surface trap states for both types of PNCs. The PL lifetime of the PNCs was measured by time-resolved photoluminescence (TRPL) spectroscopy and fit with integrated SVD-GF to determine the radiative as well as nonradiative lifetimes on the nanosecond time scale. Finally, a simple model is proposed to explain the optical and dynamic properties of the PNCs with emphasis on major exciton relaxation or electron–hole recombination processes. The results indicate that the use of capping ligand OABr resulted in PNCs with a high PL quantum yield (QY) of ∼20% (vs fluorescein, 95%), which have interesting optical properties and are promising for potential applications including photovoltaics, detectors, and light-emitting diodes (LEDs).

We present the fabrication and characterization of Ti-doped hematite (a-Fe 2 O 3 ) films for application as photoanodes in photoelectrochemical (PEC) cells for water splitting. It is demonstrated that Ti doping significantly improves the PEC activity as the photocurrent at 1.0 V vs. Ag/AgCl electrode for a 400 nm thick Ti-doped film (0.66 mA cm À2 ) was found to be $14 times higher than that of an undoped film (0.045 mA cm À2 ). The films were characterized by X-ray diffraction (XRD), Raman spectroscopy, X-ray photoelectron spectroscopy (XPS), and ultrafast transient absorption spectroscopy to obtain information about their structural, electronic, and charge carrier dynamic properties. Based on characterization of the chemical states of the involved elements as well as the charge carrier dynamics of the films with Ti doping, it appears that the photocurrent enhancement is related to an increase in charge carrier density or reduced electron-hole recombination. The highest incident photon conversion efficiency (IPCE) measured for this system was 27.0% at 360 nm at a potential of 1.23 V vs. reversible hydrogen electrode (RHE), which was obtained on a 400 nm thick Ti-doped a-Fe 2 O 3 film.

Assessing the intrinsic material performance of emerging copper-based ternary oxide photocathode candidate materials such as CuBi 2 O 4 (CBO) has been challenging due to the formation of phasesegregated domains in films with stoichiometric nonideality. However, we find films with CuO phase segregation demonstrate improved photoelectrochemical (PEC) performance, the origin of which inspired this deeper investigation. Uniform and compact CBO thin films with Bi:Cu ratios of 2.10, 1.97, 1.78, and 1.38 were grown by spin-coating. Although CuO was detected by Raman and X-ray diffraction in the 1.38 film only, high resolution energy-dispersive X-ray spectroscopy mapping revealed the presence of 10−20 nm CuO particles at the CBO/FTO interface in the 1.38, 1.78, and 1.97 samples. The greater number of CuO particles in the 1.38 sample resulted in a 25% enhancement in incident photon-to-current efficiency performance but could not be attributed to CuO-related light absorption. X-ray photoelectron spectroscopy characterization of the type-II band alignment was used to confirm that the particles behave as hole-selective contacts. The presence of nanoparticulate heterojunctions improves carrier collection of low diffusion length holes, enhancing the performance of the heterojunction beyond that of a fully planar derivative.

This work examines the effect of Zr(4+) ions on the physical and photoelectrochemical (PEC) properties of hematite (α-Fe2O3) nanorod arrays grown in an aqueous solution containing zirconyl nitrate (ZrO(NO3)2) as a dopant precursor. The concentration of ZrO(NO3)2 in the precursor solution influenced both the film thickness and the Zr(4+) concentration in the resulting films. Zr doping was found to enhance the photocurrent for water splitting; the highest photocurrent at 1.0 V vs. Ag/AgCl (0.33 mA cm(-2)) for the Zr-doped α-Fe2O3 film was approximately 7.2 times higher than that for the undoped film (0.045 mA cm(-2)). Additionally, the incident photon to current efficiency (IPCE) at 360 nm and 1.23 V vs. the reversible hydrogen electrode (RHE) increased from 3.8% to 13.6%. Ultrafast transient absorption spectroscopy suggests that Zr doping may influence PEC performance by reducing the rate of electron-hole recombination.

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