19 research outputs found
Thin Film and Powder-Based Semiconductor Photoanodes for Visible Light-Induced Water Splitting
Quantum-Confined CdTe Films Deposited by SILAR and Their Photoelectrochemical Stability in the Presence of Se<sup>2–</sup> as a Hole Scavenger
Quantum-confined CdTe films were
deposited by successive ionic
layer adsorption and reaction (SILAR) on nc-TiO<sub>2</sub> and on
a conducting oxide electrode (FTO) from aqueous solutions of Cd<sup>2+</sup> and Te<sup>2–</sup> prepared in situ under inert
atmosphere. The films were characterized with UV–visible absorption,
SEM, EDX, and XRD. CdTe<sub><i>n</i></sub> films exhibited
a zinc-blende structure and a red-shift in absorbance with increasing
SILAR cycles (<i>n</i>) consistent with quantum size effects
and featured either a mesoporous morphology on FTO or followed the
contours of the titania nanoparticles on nc-TiO<sub>2</sub> films.
The films’ photoelectrochemical behavior was studied in the
presence of Se<sup>2–</sup> compared to S<sup>2–</sup> as hole scavengers. The incident-photon-to-current conversion efficiency
reached ca. 16% at 460 nm and 9% at 500 nm at CdTe<sub>10</sub>/nc-TiO<sub>2</sub> in alkaline Se<sup>2–</sup> electrolyte compared to
1% at 460 nm or 0.5% at 500 nm in S<sup>2–</sup>. CdTe<sub>10</sub> films examined after acquiring a photoaction spectrum in
Se<sup>2–</sup> still exhibited zinc-blende structure, EDX
analysis showed Cd and Te peaks and no detectable Se, and the absorbance
slightly increased with films remaining red-black. On the other hand,
the absorbance edge and photocurrent onset shifted significantly to
the blue and the films became yellow during the same measurement in
S<sup>2–</sup>, indicating dissolution and formation of CdS,
consistent with reports for CdTe single crystals and Q-CdTe. After
hours of illumination at 500 nm at −0.55 V in Se<sup>2–</sup>, Se became incorporated in the films; however, the photocurrent
decreased by only 5–8% after 2–3 h illumination, indicating
significant photoelectrochemical stability. The results are attributed
to effective quenching of the anodic dissolution of CdTe by Se<sup>2–</sup> scavenging the hole, and a slow growth of a protective
overlayer possibly of CdTe<sub>1–<i>x</i></sub>Se<sub><i>x</i></sub> that does not block photocurrent generation,
in contrast to the behavior of CdTe in sulfide electrolyte
Amplification in Light Energy Conversion at Q‑CdTe Sensitized TiO<sub>2</sub> Photonic Crystal, Photoelectrochemical Stability in Se<sup>2–</sup> Electrolyte, and Size-Dependent Type II Q‑CdTe/CdSe Formation
This study investigates the ability
of Se<sup>2–</sup> redox
electrolyte to separate the photoholes and stabilize Q-CdTe quantum
dot solar cell with a liquid junction. We examined the photophysical
and photoelectrochemical behaviors of Q-CdTe in two sizes, green-emitting
dots of 2.3–2.7 nm diameter and red-emitting dots of 4 nm diameter,
in the presence of alkaline Se<sup>2–</sup> electrolyte prepared
under inert atmosphere. Photoelectrochemical, absorbance, emission
and emission quenching measurements revealed the presence of size
dependence in Se<sup>2–</sup> surface binding to Q-CdTe, growth
of type II Q-CdTe/CdSe, and stability in the photoelectrochemical
cell. Emission quenching measurements show that Se<sup>2–</sup> scavenges the Q-CdTe photohole, with mechanisms that depended on
size and quencher concentration. Binding of Se<sup>2–</sup> to green-emitting Q-CdTe occurred with a greater binding constant
compared to the red-emitting dots, resulting in formation of type
II Q-CdTe/CdSe at the smaller core indicated in red-shifted absorbance
and emission spectra with incremental Se<sup>2–</sup> addition
at room temperature. Photoelectrochemical measurements acquired at
Q-CdTe sensitized nc-TiO<sub>2</sub> and TiO<sub>2</sub> inverse opal
with a stop band at 600 nm, 600-i-TiO<sub>2</sub>-o, in Se<sup>2–</sup> electrolyte confirmed this redox species ability to scavenge the
photohole and to protect Q-CdTe against fast photoanodic dissolution,
with greater stability observed for the larger dots. Gains in the
photon-to-current conversion efficiency attributed to light trapping
were measured at Q-CdTe sensitized 600-i-TiO<sub>2</sub>-o relative
to nc-TiO<sub>2</sub>
Yttrium Tantalum Oxynitride Multiphases as Photoanodes for Water Oxidation
The perovskite yttrium tantalum oxynitride is theoretically proposed as a promising semiconductor for solar water splitting because of the predicted band gap and energy positions of band edges. In experiments, however, we show here that depending on the processing parameters, yttrium tantalum oxynitrides exist in multi phases, including the desired perovskite YTaON2, defect fluorite YTa(O,N,square)(4), and N-doped YTaO4. These multiphases have band gaps ranging between 2.13 and 2.31 eV, all responsive to visible light. The N-doped YTaO4, perovskite main phase, and fluorite main phase derived from crystalline fergusonite oxide precursors exhibit interesting photoelectrochemical performances for water oxidation, while the defect fluorite derived from low-crystallized scheelite-type oxide precursors shows negligible activity. Preliminary measurements show that loading an IrOx, cocatalyst on N-doped YTaO4 significantly improves its photoelectrochemical performance, encouraging further studies to optimize this new material for solar fuel production
Black-Si as a Photoelectrode
The fabrication and characterization of photoanodes based on black-Si (b-Si) are presented using a photoelectrochemical cell in NaOH solution. B-Si was fabricated by maskless dry plasma etching and was conformally coated by tens-of-nm of TiO2 using atomic layer deposition (ALD) with a top layer of CoO x cocatalyst deposited by pulsed laser deposition (PLD). Low reflectivity R < 5 % of b-Si over the entire visible and near-IR ( λ < 2 μ m) spectral range was favorable for the better absorption of light, while an increased surface area facilitated larger current densities. The photoelectrochemical performance of the heterostructured b-Si photoanode is discussed in terms of the n-n junction between b-Si and TiO2