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At least 271 records · Page 15

Tandem Core–Shell Si–Ta 3 N 5 Photoanodes for Photoelectrochemical Water Splitting

Here, nanostructured core–shell Si–Ta 3 N 5 photoanodes were designed and synthesized to overcome charge transport limitations of Ta 3 N 5 for photoelectrochemical water splitting. The core–shell devices were fabricated by atomic layer deposition of amorphous Ta 2 O 5 onto nanostructured Si and subsequent nitridation to crystalline Ta 3 N 5 . Nanostructuring with a thin shell of Ta 3 N 5 results in a 10-fold improvement in photocurrent compared to a planar device of the same thickness. In examining thickness dependence of the Ta 3 N 5 shell from 10 to 70 nm, superior photocurrent and absorbed-photon-to-current efficiencies are obtained from the thinner Ta 3 N 5 shells, indicating minority carrier diffusion lengths on the order of tens of nanometers. The fabrication of a heterostructure based on a semiconducting, n-type Si core produced a tandem photoanode with a photocurrent onset shifted to lower potentials by 200 mV. CoTiO x and NiO x water oxidation cocatalysts were deposited onto the Si–Ta 3 N 5 to yield active photoanodes that with NiO x retained 50–60% of their maximum photocurrent after 24 h chronoamperometry experiments and are thus among the most stable Ta 3 N 5 photoanodes reported to date.

36 MATERIALS SCIENCE↗

Investigation of p-type Ca 2 Fe 2 O 5 as a Photocathode for Use in a Water Splitting Photoelectrochemical Cell

Ca 2 Fe 2 O 5 is a p-type oxide that has not been previously investigated as a photocathode for use in a water splitting photoelectrochemical cell. In this study, Ca 2 Fe 2 O 5 was synthesized as a polycrystalline electrode, and its properties relevant to photoelectrochemical hydrogen production were investigated. Ca 2 Fe 2 O 5 electrodes were prepared by thermally annealing electrodeposited FeOOH films with a solution of Ca(NO 3 ) 2 drop-casted onto the electrode surface. The bandgap energy, band edge positions, flatband potential, photocurrent generation, and chemical and photoelectrochemical stabilities of Ca 2 Fe 2 O 5 were examined. The results showed that Ca 2 Fe 2 O 5 has an ideal bandgap and band positions that can enable the utilization of visible light for overall solar water splitting. Photocurrent-time measurements were also performed and the changes in morphology, crystallinity, and composition of the Ca 2 Fe 2 O 5 electrodes before and after the photocurrent measurement were investigated. Furthermore, this made it possible to examine the photostability of Ca 2 Fe 2 O 5 and elucidate the cause of the observed photocurrent decay.

25 ENERGY STORAGE↗

Photoelectrochemical Properties and Stability of Nanoporous p-Type LaFeO 3 Photoelectrodes Prepared by Electrodeposition

LaFeO 3 is a p-type oxide that has an ideal bandgap and band edge positions for overall solar water splitting. This study reports an electrochemical synthesis method to produce LaFeO 3 as a high surface area, nanoporous photocathode. The resulting electrode generated a photocurrent density of 0.1 mA/cm 2 at a potential as positive as 0.73 V vs. RHE for photoelectrochemical oxygen reduction with a photocurrent onset potential very close to its flatband potential of 1.45 V vs. RHE. Furthermore, without a protection layer it showed a stable photocurrent generation with no sign of photocorrosion. Due to the poor catalytic nature of the LaFeO 3 surface for water reduction, photocurrent obtained for water reduction was not substantial. Furthermore, its photostability and its ability to achieve a photovoltage for water reduction greater than 1.2 V encourage further studies on doping to enhance electron-hole separation as well as interfacing appropriate hydrogen evolution catalysts.

37 INORGANIC, ORGANIC, PHYSICAL, AND ANALYTICAL CH↗

Rapid Flame-Annealed CuFe 2 O 4 as Efficient Photocathode for Photoelectrochemical Hydrogen Production

Copper ferrite (CuFe 2 O 4 ) possesses an indirect bandgap in the range of 1.54–1.95 eV. It is used as an attractive p-type photocathode in photoelectrochemical (PEC) water splitting, and theoretically it can yield a maximum photocurrent density of ~27 mA/cm 2 and a maximum solar-to-hydrogen conversion efficiency of ~33%. To date, only a few reports have been published on CuFe 2 O 4 photocathodes with very low-photocurrent densities, with a maximum value of 0.4 mA/cm2 at 0.4 V vs RHE. Herein, we prepared a CuFe 2 O 4 photocathode on FTO glass with the sol–gel method followed by either high-temperature flame annealing or furnace annealing. We found that the flame-annealed CuFe 2 O 4 photocathode generated a photocurrent density of 1.82 mA/cm 2 at 0.4 V vs RHE that is approximately 3.5 times higher than the furnace-annealed CuFe 2 O 4 (0.52 mA/cm 2 ). This photocurrent density is also higher than those of all the reported CuFe 2 O 4 photocathodes, and any Cu containing ternary oxide (Cu–M–O, M: Fe, Bi, V, and Nb) photocathode (0.1–1.3 mA/cm 2 at 0.4 V vs RHE). An improved PEC performance of the flame-annealed CuFe 2 O 4 photocathode is elicited owing to the beneficial effects of flame annealing on the physical, optical, and electrical properties of CuFe 2 O 4 . Flame annealing enhances the light absorption property of the CuFe 2 O 4 photocathode by slightly reducing the bandgap, and by forming a thicker film with increased porosity. Flame annealing also reduces the oxygen vacancy concentration in CuFe 2 O 4 , thus facilitating charge transport and interfacial charge transfer processes. Moreover, flame annealing requires only 16 min, which is much shorter than the time required for furnace annealing (~9 h). Furthermore, these results demonstrate that flame annealing is a rapid and effective means for fabricating metal oxide photoelectrodes with an enhanced PEC water splitting performance.

37 INORGANIC, ORGANIC, PHYSICAL, AND ANALYTICAL CH↗

Hot Electron-driven Photocatalysis and Transient Absorption Spectroscopy in Plasmon Resonant Grating Structures

Plasmon resonant grating structures provide an effective platform for distinguishing between the effects of plasmon resonant excitation and bulk metal absorption via interband transitions. By simply rotating the polarization of the incident light, we can switch between resonant excitation and non-resonant excitation, while keeping all other parameters of the measurement constant. With light polarized perpendicular to the lines in the grating (i.e., TE-polarization), the photocatalytic reaction rate (i.e., photocurrent) is measured as the angle of the incident laser light is tuned through the resonance with the grating. Here, hot holes photoexcited in the metal are used to drive the oxygen evolution reaction (OER), producing a measurable photocurrent. Using TE-polarized light, we observe sharp peaks in the photocurrent and sharp dips in the photoreflectance at approximately 9° from normal incidence, which corresponds to the conditions under which there is good wavevector matching between the incident light and the lines in the grating. With light polarized parallel to the grating (i.e., TM), we excite the grating structure non-resonantly and there is no angular dependence in the photocurrent or photoreflectance. In order to quantify the lifetime of these hot carriers, we performed transient absorption spectroscopy of these plasmon resonant grating structures. Here, we observe one feature in the spectra corresponding to interband transitions and another feature associated with the plasmon resonant mode in the grating. Both features decay over a time scale of 1–2 ps. Finally, the spectral responses of grating structures fabricated with Ag, Al, and Cu are also presented.

37 INORGANIC, ORGANIC, PHYSICAL, AND ANALYTICAL CH↗

ZnO/anthracene based inorganic/organic nanowire heterostructure: Photoresponse and photoluminescence studies

The effects of surface modification of vertically aligned ZnO nanowires (NWs) with anthracene for the improved photocurrent, photoresponse, and UV photoluminescence have been investigated in this work. The formation of ZnO/anthracene based inorganic/organic NWs heterostructure by surface capping with anthracene solution was confirmed from the high resolution transmission electron microscopy and Fourier transport infrared spectroscopy analyses. After the anthracene capping of ZnO NWs, despite an increase in dark current, we obtained a significant improvement in the photocurrent and photoresponsivity. A sixfold improvement in the UV photocurrent-to-dark current ratio is obtained with capping. Compared to the uncapped NWs, the photoresponse is significantly faster for the ZnO/anthracene system with response and reset times of 1.5 and 1.6 s, respectively. The room temperature photoluminescence spectra show threefold enhanced UV emission with large enhancement in the ratio of UV to green emission intensities. The faster photoresponse and enhanced photocurrent from the ZnO/anthracene heterostructure are explained on the basis of modification of surface defects and interfacial charge transfer process.

36 MATERIALS SCIENCE↗

Enhanced photodetection in graphene-integrated photonic crystal cavity

We demonstrate the controlled enhancement of photoresponsivity in a graphene photodetector by coupling to slow light modes in a long photonic crystal linear defect cavity. Near the Brillouin zone (BZ) boundary, spectral coupling of multiple cavity modes results in broad-band photocurrent enhancement from 1530 nm to 1540 nm. Away from the BZ boundary, individual cavity resonances enhance the photocurrent eight-fold in narrow resonant peaks. Optimization of the photocurrent via critical coupling of the incident field with the graphene-cavity system is discussed. The enhanced photocurrent demonstrates the feasibility of a wavelength-scale graphene photodetector for efficient photodetection with high spectral selectivity and broadband response.

36 MATERIALS SCIENCE↗

Balancing high gain and bandwidth in multilayer organic photodetectors with tailored carrier blocking layers

We present detailed studies of the high photocurrent gain behavior in multilayer organic photodiodes containing tailored carrier blocking layers we reported earlier in a Letter [W. T. Hammond and J. Xue, Appl. Phys. Lett. 97, 073302 (2010)], in which a high photocurrent gain of up to 500 was attributed to the accumulation of photogenerated holes at the anode/organic active layer interface and the subsequent drastic increase in secondary electron injection from the anode. Here, we show that both the hole-blocking layer structure and layer thickness strongly influence the magnitude of the photocurrent gain. Temporal studies revealed that the frequency response of such devices is limited by three different processes with lifetimes of 10 μs, 202 μs, and 2.72 ms for the removal of confined holes, which limit the 3 dB bandwidth of these devices to 1.4 kHz. Furthermore, the composition in the mixed organic donor-acceptor photoactive layer affects both gain and bandwidth, which is attributed to the varying charge transport characteristics, and the optimal gain-bandwidth product is achieved with approximately 30% donor content. Finally, these devices show a high dynamic range of more than seven orders of magnitude, although the photocurrent shows a sublinear dependence on the incident optical power.

46 INSTRUMENTATION RELATED TO NUCLEAR SCIENCE AND ↗

Localized surface plasmon induced enhancement of electron-hole generation with silver metal island at n-Al:ZnO/p-Cu{sub 2}O heterojunction

Localized surface plasmon induced generation of electron-hole pairs with inclusion of metal islands of noble metal like Ag can enhance the photocurrent. A heterostructure of n-Al:ZnO/p-Cu{sub 2}O with inclusion of Ag metalislands at the junction has been fabricated. I-V characteristic curve of these heterostructures shows a significant enhancement of photocurrent under the illumination (1.5 AMU). This enhancement of photocurrent is attributed to the supply of hot electrons generated in silver metal nanoislands. It has also been shown that inclusion of metal islands increases the absorption of solar spectrum in visible region at 500 nm. Enhancement of photocurrent may also be due to the direct resonance energy transfer from Localized Surface Plasmons of metal islands to Cu{sub 2}O.

71 CLASSICAL AND QUANTUM MECHANICS, GENERAL PHYSIC↗

Plasmon resonant amplification of hot electron-driven photocatalysis

We discuss plasmon resonant excitation of hot electrons in a metal based photocatalyst in the oxygen evolution half reaction in aqueous solution. In this report, the photocatalyst consists of a 100-nm thick Au film deposited on a corrugated silicon substrate. Here, hot electrons photoexcited in the metal are injected into the solution, ultimately reversing the water oxidation reaction (O 2 +4H + +4e–⇌2H 2 O) and producing a photocurrent. In order to amplify this process, the gold electrode is patterned into a plasmon resonant grating structure with a pitch of 500 nm. The photocurrent (i.e., charge transfer rate) is measured as a function of incident angle using 633 nm wavelength light. We observe peaks in the photocurrent at incident angles of ±9° from normal when the light is polarized parallel to the incident plane (p-polarization) and perpendicular to the lines on the grating. Due to these peaks, we estimate an overall plasmonic gain (or amplification) factor of 2.1× in the charge transfer rate. At these same angles, we also observe sharp dips in the photoreflectance, corresponding to the condition when there is wavevector matching between the incident light and the plasmon mode in the grating. No angle dependence is observed in the photocurrent or photoreflectance when the incident light is polarized perpendicular to the incident plane (s-polarization) and parallel to the lines on the grating. Finite difference time domain simulations also predict sharp dips in the photoreflectance at ±9°, and the electric field intensity profiles show clear excitation of a plasmon-resonant mode when illuminated at those angles with p-polarized light.

42 ENGINEERING↗

Effect of wavefunction delocalization on shift current generation

We derive upper bounds on the magnitude of shift photocurrent generation of materials in two limiting cases: the flat-band limit of almost-isolated systems such as molecular crystals, and the wide-band limit of one-dimensional or quasi-one-dimensional materials such as ferroelectric polymers or other materials with chain-like motifs. These bounds relate the magnitudes of the shift current bulk photovoltaic effect to materials parameters. In both cases, we find that ratio of electron hopping amplitudes to the band gap plays a vital role in maximizing the amount of nonlinear response. Furthermore, by using the Wannier function formalism, we quantify the effect of long-range hopping amplitudes, showing how delocalization of electronic states gives rise to larger photocurrents. Lastly, these results inform the design and selection of new materials for large shift current generation.

75 CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND↗

Bulk photovoltaic effects in the presence of a static electric field

This paper presents a study of dc photocurrents in biased insulators to the third order in the electric field. Here, we find three photocurrents which are characterized by physical divergences of the third-order free-electron polarization susceptibility. In the absence of momentum relaxation and saturation effects, these dc photocurrents grow as t n (n = 2, 1, 0) with illumination time. The photocurrents are dubbed jerk, third-order injection, and third-order shift current, respectively, and are generalizations of the second-order injection and shift currents of the bulk photovoltaic effect (BPVE). We also revisit the theory of the second-order bulk photovoltaic effect and include Fermi surface contributions which are important in metals. Finally, we show that injection, shift, and jerk currents admit simple physical interpretations in terms of semiclassical wave packet dynamics in electric fields. Experimental signatures and extensions to higher-order susceptibilities are also discussed.

75 CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND↗

Competing Channels for Hot-Electron Cooling in Graphene

We report here on temperature-dependent photocurrent measurements of high-quality dual-gated monolayer graphene p - n junction devices. A photothermoelectric effect governs the photocurrent response in our devices, allowing us to track the hot-electron temperature and probe hot-electron cooling channels over a wide temperature range (4 to 300 K). At high temperatures ( T > T * ), we found that both the peak photocurrent and the hot spot size decreased with temperature, while at low temperatures ( T < T * ), we found the opposite, namely that the peak photocurrent and the hot spot size increased with temperature. This nonmonotonic temperature dependence can be understood as resulting from the competition between two hot-electron cooling pathways: (a) (intrinsic) momentum-conserving normal collisions that dominates at low temperatures and (b) (extrinsic) disorder-assisted supercollisions that dominates at high temperatures. Gate control in our high-quality samples allows us to resolve the two processes in the same device for the first time. The peak temperature T * depends on carrier density and disorder concentration, thus allowing for an unprecedented way of controlling graphene’s photoresponse.

36 MATERIALS SCIENCE↗

Electrolyte Concentration Effect of a Photoelectrochemical Cell Consisting of TiO 2 Nanotube Anode

The photoelectrochemical responses of a TiO 2 nanotube anode in ethylene glycol (EG), glycerol, ammonia, ethanol, urea, and Na 2 S electrolytes with different concentrations were investigated. The TiO 2 nanotube anode was highly efficient in photoelectrocatalysis in these solutions under UV light illumination. The photocurrent density is obviously affected by the concentration change. Na 2 S generated the highest photocurrent density at 0, 1, and 2 V bias voltages, but its concentration does not significantly affect the photocurrent density. Urea shows high open circuit voltage at proper concentration and low photocurrent at different concentrations. Externally applied bias voltage is also an important factor that changes the photoelectrochemical reaction process. In view of the open circuit voltage, EG, ammonia, and ethanol fuel cells show the trend that the open circuit voltage (OCV) increases with the increase of the concentration of the solutions. Glycerol has the highest OCV compared with others, and it deceases with the increase in the concentration because of the high viscosity. The OCV of the urea and Na 2 S solutions did not show obvious concentration effect.

Ren, Kai↗

Substituent effects on the electrical conductivities of the phenazine derivatives

The and/or photoconductivities of 16 substituted phenazines having methoxy, hydroxy, chloro, nitro, amino or t-butyl group at 1-, 2-, 1, 6- or 2,7- positions of the phenazine ring measured by using the surface type cells. The energy gaps of the dark conductivities in the range 2.0 to 2.3 were independent of the kinds and the positions of the substituent groups, although the photo-absorption wavelength of the evaporated films changed with them. No correlation between photoconductivity and fluorescence was observed. The photocurrent was affected by the position of the substituents; namely, the photocurrents of the 1,6-di-substituted phenazines. When the substituent at 1,6-positions was hydroxy or amino group, however, the photocurrents decreased. The photocurrents decreased drastically in the presence of oxygen.

Sugimoto, A.↗

Electrochemical performance and enhanced photocatalytic activity of Ce-doped BiVO{sub 4} under visible light irradiation

Highlights: • Ce-BiVO{sub 4} was synthesized via a simple precipitation-impregnation method. • Photo-generated electrons transfer from the BiVO{sub 4} to the Ce{sup 4+} ions. • The enhanced interfacial electron transfer for Ce-BiVO{sub 4} was observed using EIS and photocurrent. • The enhanced activity of Ce-BiVO{sub 4} is mainly attributed to the increased charge separation. - Abstract: Ce-BiVO{sub 4} composites have been synthesized via a simple precipitation-impregnation method and were characterized using X-ray diffraction (XRD), scanning electron microscopy (SEM), X-ray photoelectron spectroscopy (XPS), UV–vis diffuse reflectance spectrum (DRS), electrochemical impedance spectrum (EIS) and photocurrent. All the BiVO{sub 4} and Ce-BiVO{sub 4} samples are composed of monoclinic scheelite BiVO{sub 4}. Compared to BiVO{sub 4}, the increased photocurrent and decreased diameter of the semicircle have been observed for Ce-BiVO{sub 4}, indicating that the Ce-doping can enhance interfacial electron transfer for Ce-BiVO{sub 4}. Ce-BiVO{sub 4} composites show enhanced activity in the photocatalytic degradation of rhodamine B under visible light irradiation in comparison with P25 and pure BiVO{sub 4}, and 1.0%Ce-BiVO{sub 4} shows the best photocatalytic activity because of its enhanced light absorption, narrowed bandgap and improved separation of the photogenerated electron–hole pairs, which was achieved as a result of photogenerated electrons transfer from the BiVO{sub 4} to the Ce{sup 4+} ions.

36 MATERIALS SCIENCE↗

Low cost and facile fabrication of broadband laser power meter based on reduced graphene oxide film

Highlights: • The reduced graphene oxide film is used to fabricate the low cost laser powermeter. • The photoresponse of the device is explored in the visible to near-infrared range. • The photoresponse of the device is linearly related to the irradiated laser power. • The photoelectric current of the device does not depend on the laser spot size. - Abstract: Here, we have demonstrated a new type of broadband reduced graphene oxide-based laser power meter in simple and low cost method. The broadband photosensitivity of the device is confirmed by photocurrent measurements at different incident laser wavelengths of 405, 532, 635 and 808 nm. It is shown that its photocurrent increases linearly with increasing the power of the laser beam. Also, it is observed that the photocurrent behavior of the device does not depend upon the size of the laser spot. It should be noted that the reduced graphene oxide power meter is the thermal detection device. Therefore, the response of the sample in the vacuum is greatly enhanced in compared to the environmental air. Cooling system can also decrease the time required for the establishment of thermal equilibrium and thus reduce the response time of the power meter. These results open up exciting opportunities for developing broadband photodetectors.

75 CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND↗

Study the performance of photogalvanic cells for solar energy conversion and storage: Rose Bengal-D-Xylose-NaLS system

The Rose Bengal is used as photosensitizer with D-Xylose as reductant and sodium lauryl sulphate (NaLS) as surfactant for the enhancement of the conversion efficiency and storage capacity of photogalvanic cell for its commercial viability. The observed value of the photogeneration of photopotential was 885.0 mV and photocurrent was 460.0 {mu}A whereas maximum power of the cell was 407.10 {mu}W. The observed power at power point was 158.72 {mu}W and the conversion efficiency was 1.52%. The fill factor 0.3151 was experimentally determined at the power point of the cell. The rate of initial generation of photocurrent was 63.88 {mu}A min{sup -1}. The photogalvanic cell so developed can work for 145.0 min in dark on irradiation for 165.0 min, i.e. the storage capacity of the photogalvanic cell is 87.87%. A simple mechanism for the photogeneration of photocurrent has also been proposed. (author)

14 SOLAR ENERGY↗