Abstract:Severe interfacial electron–hole recombination greatly limits the performance of CuWO4 photoanode towards the photoelectrochemical (PEC) oxygen evolution reaction (OER). Surface modification with an OER cocatalyst can reduce electron–hole recombination and thus improve the PEC OER performance of CuWO4. Herein, we coupled CuWO4 nanoflakes (NFs) with Iridium–cobalt phosphates (IrCo-Pi) and greatly improved the photoactivity of CuWO4. The optimized photocurrent density for CuWO4/IrCo-Pi at 1.23 V vs. reversible h… Show more
“…The transient photocurrent response to the on/off illumination as well as its decay mainly depend on the photogeneration/relaxation mechanism of the e – /h + pairs. − The initially originated photocurrent ( I i ) upon illumination can be attributed to the separation of photogenerated charge carriers at the semiconductor/electrolyte interface (SEI). Then, the photogenerated electrons transfer to the back contact, while the photoinduced holes move to the electrolyte to oxidize H 2 O. ,− By this time, a gradual decrease of the photocurrent is established until reaching a steady-state photocurrent ( I f ). , The photocurrent decay indicates charge carriers recombination. Upon light-off condition, the trapped holes at the semiconductor surface and the photogenerated electrons recombine. , The transient photocurrent can be calculated using eq : where t is the time, τ is the transient time constant, and the parameter D is given by eq :where I t is the current at any time t , I i is the initial spike current, and I f is the steady-state current.…”
Section: Resultsmentioning
confidence: 99%
“…Then, the photogenerated electrons transfer to the back contact, while the photoinduced holes move to the electrolyte to oxidize H 2 O. ,− By this time, a gradual decrease of the photocurrent is established until reaching a steady-state photocurrent ( I f ). , The photocurrent decay indicates charge carriers recombination. Upon light-off condition, the trapped holes at the semiconductor surface and the photogenerated electrons recombine. , The transient photocurrent can be calculated using eq : where t is the time, τ is the transient time constant, and the parameter D is given by eq :where I t is the current at any time t , I i is the initial spike current, and I f is the steady-state current. The transient time constant (τ) might be considered as the charge carrier’s lifetime and generally could be described as the time at which ln D = −1, as shown in Figure b. ,, It is worth mentioning that when the transient time constant increased, the recombination processes get delayed.…”
Section: Resultsmentioning
confidence: 99%
“…98,100−102 By this time, a gradual decrease of the photocurrent is established until reaching a steady-state photocurrent (I f ). 103,104 The photocurrent decay indicates charge carriers recombination. Upon light-off condition, the trapped holes at the semiconductor surface and the photogenerated electrons recombine.…”
mentioning
confidence: 99%
“…Upon light-off condition, the trapped holes at the semiconductor surface and the photogenerated electrons recombine. 103,104 The transient photocurrent can be calculated using eq 5: 96…”
Designing efficient and stable water
splitting photocatalysts is
an intriguing challenge for energy conversion systems. We report on
the optimal fabrication of perfectly aligned nanotubes on trimetallic
Ti–Mo–Fe alloy with different compositions prepared
via the combination of metallurgical control and facile electrochemical
anodization in organic media. The X-ray diffraction (XRD) patterns
revealed the presence of composite oxides of anatase TiO2 and magnetite Fe3O4 with better stability
and crystallinity. With the optimal alloy composition Ti–(5.0
atom %) Mo–(5.0 atom %) Fe anodized for 16 h, enhanced conductivity,
improved photocatalytic performance, and remarkable stability were
achieved in comparison with Ti–(3.0 atom %) Mo–(1.0
atom %) Fe samples. Such optimized nanotube films attained an enhanced
photocatalytic activity of ∼0.272 mA/cm2 at 0.9
VSCE, which is approximately 4 times compared to the bare
TiO2 nanotubes fabricated under the same conditions (∼0.041
mA/cm2 at 0.9 VSCE). That was mainly correlated
with the emergence of Mo and Fe impurities within the lattice, providing
excess charge carriers. Meanwhile, the nanotubes showed outstanding
stability with a longer electron lifetime. Moreover, carrier density
variations, lower charge transfer resistance, and charge carriers
dynamics features were demonstrated via the Mott–Schottky and
electrochemical impedance analyses.
“…The transient photocurrent response to the on/off illumination as well as its decay mainly depend on the photogeneration/relaxation mechanism of the e – /h + pairs. − The initially originated photocurrent ( I i ) upon illumination can be attributed to the separation of photogenerated charge carriers at the semiconductor/electrolyte interface (SEI). Then, the photogenerated electrons transfer to the back contact, while the photoinduced holes move to the electrolyte to oxidize H 2 O. ,− By this time, a gradual decrease of the photocurrent is established until reaching a steady-state photocurrent ( I f ). , The photocurrent decay indicates charge carriers recombination. Upon light-off condition, the trapped holes at the semiconductor surface and the photogenerated electrons recombine. , The transient photocurrent can be calculated using eq : where t is the time, τ is the transient time constant, and the parameter D is given by eq :where I t is the current at any time t , I i is the initial spike current, and I f is the steady-state current.…”
Section: Resultsmentioning
confidence: 99%
“…Then, the photogenerated electrons transfer to the back contact, while the photoinduced holes move to the electrolyte to oxidize H 2 O. ,− By this time, a gradual decrease of the photocurrent is established until reaching a steady-state photocurrent ( I f ). , The photocurrent decay indicates charge carriers recombination. Upon light-off condition, the trapped holes at the semiconductor surface and the photogenerated electrons recombine. , The transient photocurrent can be calculated using eq : where t is the time, τ is the transient time constant, and the parameter D is given by eq :where I t is the current at any time t , I i is the initial spike current, and I f is the steady-state current. The transient time constant (τ) might be considered as the charge carrier’s lifetime and generally could be described as the time at which ln D = −1, as shown in Figure b. ,, It is worth mentioning that when the transient time constant increased, the recombination processes get delayed.…”
Section: Resultsmentioning
confidence: 99%
“…98,100−102 By this time, a gradual decrease of the photocurrent is established until reaching a steady-state photocurrent (I f ). 103,104 The photocurrent decay indicates charge carriers recombination. Upon light-off condition, the trapped holes at the semiconductor surface and the photogenerated electrons recombine.…”
mentioning
confidence: 99%
“…Upon light-off condition, the trapped holes at the semiconductor surface and the photogenerated electrons recombine. 103,104 The transient photocurrent can be calculated using eq 5: 96…”
Designing efficient and stable water
splitting photocatalysts is
an intriguing challenge for energy conversion systems. We report on
the optimal fabrication of perfectly aligned nanotubes on trimetallic
Ti–Mo–Fe alloy with different compositions prepared
via the combination of metallurgical control and facile electrochemical
anodization in organic media. The X-ray diffraction (XRD) patterns
revealed the presence of composite oxides of anatase TiO2 and magnetite Fe3O4 with better stability
and crystallinity. With the optimal alloy composition Ti–(5.0
atom %) Mo–(5.0 atom %) Fe anodized for 16 h, enhanced conductivity,
improved photocatalytic performance, and remarkable stability were
achieved in comparison with Ti–(3.0 atom %) Mo–(1.0
atom %) Fe samples. Such optimized nanotube films attained an enhanced
photocatalytic activity of ∼0.272 mA/cm2 at 0.9
VSCE, which is approximately 4 times compared to the bare
TiO2 nanotubes fabricated under the same conditions (∼0.041
mA/cm2 at 0.9 VSCE). That was mainly correlated
with the emergence of Mo and Fe impurities within the lattice, providing
excess charge carriers. Meanwhile, the nanotubes showed outstanding
stability with a longer electron lifetime. Moreover, carrier density
variations, lower charge transfer resistance, and charge carriers
dynamics features were demonstrated via the Mott–Schottky and
electrochemical impedance analyses.
“…4−6 However, poor bulk charge transport and surface water oxidation activity limit the performance of CuWO 4 for PEC water splitting. 5,7 Many studies have been conducted on doping, 8,9 oxygen vacancies, 10−12 heterojunctions 13−15 and cocatalysts 16,17 to optimize its existing problems. 13,14,17−19 Doping with other elements can improve the conductivity by increasing the carrier density.…”
Hydrogen generation through photoelectrochemical (PEC) technology is one of the most appropriate ways for delivering sustainable fuel. Simultaneously, anisotropic properties will be exhibited by the materials with low crystal symmetry, allowing the tuning of the PEC properties by controlling the crystallographic orientation and exposed facets. Therefore, we synthesized copper tungstate films (CuWO 4 ) with highly exposed (100) crystal facets by regulating anions in the precursor solution. According to experimental characterization and density functional theory calculations, the CuWO 4 film with a high exposure ratio of the (100) crystal facet has promoted charge transport with trapfree mode and reduced recombination of electrons and holes. Meanwhile, the oxygen evolution reaction is promoted on the (100) facet because of the relatively low energy barrier. Compared to the CuWO 4 with other mixed exposure facets, CuWO 4 with a highly exposed (100) facet presents a twofold current density (0.38 mA/cm 2 ) and one-fifteenth electron transit time (0.698 ms) and also has great stability (more than 6 h). These results provide an easy way to enhance the PEC performance by modulating the exposure facets of the film electrode.
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