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Photoelectrochemistry with the optical rotating disc electrode - Part 2. Steady-state and transient studies on colloidal CdS

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Photoelectrochemistry with the optical rotating disc electrode - Part 2. Steady-state and transient studies on colloidal CdS. / Boxall, C ; Albery, W. John .
In: Physical Chemistry Chemical Physics, Vol. 2, No. 16, 2000, p. 3641-3650.

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Boxall C, Albery WJ. Photoelectrochemistry with the optical rotating disc electrode - Part 2. Steady-state and transient studies on colloidal CdS. Physical Chemistry Chemical Physics. 2000;2(16):3641-3650. doi: 10.1039/B001338M

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Boxall, C ; Albery, W. John . / Photoelectrochemistry with the optical rotating disc electrode - Part 2. Steady-state and transient studies on colloidal CdS. In: Physical Chemistry Chemical Physics. 2000 ; Vol. 2, No. 16. pp. 3641-3650.

Bibtex

@article{bea910493a4f48f18cc23c656897a6b6,
title = "Photoelectrochemistry with the optical rotating disc electrode - Part 2. Steady-state and transient studies on colloidal CdS",
abstract = "Results are presented for the dark and photoelectrochemistry of colloidal CdS particles studied with the optical rotating disc electrode (ORDE). The behaviour of the particles in the dark is governed by reversible electron transfer from a range of surface states superimposed over reversible electron transfer direct from the particle conduction band or shallow electron traps just below the conduction band edge. The oxidative current due to the latter effect exhibits a range of onset potentials arising from the polydisperse, Q-state nature of the particles under interrogation. The steady-state photoelectrochemistry varies from that in the dark in that (i) the surface states play a different role in determining the shape of the current voltage curve as they have been mostly oxidised by photogenerated valence band holes; and (ii) the photocurrent onset shifts to more anodic potentials as a result of a surface state-driven photocurrent attenuation and positive charge accumulation at the particle surface, both derived from hole-driven surface state oxidation. Light-on transient photocurrent measurements with the ORDE allow calculation of a pseudo-first-order rate coefficient for photogenerated electron loss, k(0), of similar to 0.07 s(-1). This suggests that the loss process being interrogated is not photogenerated electron-valence band hole recombination, but the loss of electrons left on the particle after some valence band hole filling reaction has occurred. Transient experiments also allow calculation of phi, the quantum efficiency for the photogeneration of electrons detectable by the ORDE. phi is found to be similar to 0.006, indicating that the dominant processes within the particle are direct and indirect photogenerated electron-valence band hole recombination.",
keywords = "SMALL SEMICONDUCTOR PARTICLES, CHARGE-TRANSFER PROCESSES, LIQUID-SOLID INTERFACE, CADMIUM-SULFIDE, PHOTOREDOX REACTIONS, RADIATION-CHEMISTRY, TRAPPED ELECTRONS, OXIDE COLLOIDS, PHOTOCHEMISTRY, FEMTOSECOND",
author = "C Boxall and Albery, {W. John}",
year = "2000",
doi = "10.1039/B001338M",
language = "English",
volume = "2",
pages = "3641--3650",
journal = "Physical Chemistry Chemical Physics",
issn = "1463-9076",
publisher = "Royal Society of Chemistry",
number = "16",

}

RIS

TY - JOUR

T1 - Photoelectrochemistry with the optical rotating disc electrode - Part 2. Steady-state and transient studies on colloidal CdS

AU - Boxall, C

AU - Albery, W. John

PY - 2000

Y1 - 2000

N2 - Results are presented for the dark and photoelectrochemistry of colloidal CdS particles studied with the optical rotating disc electrode (ORDE). The behaviour of the particles in the dark is governed by reversible electron transfer from a range of surface states superimposed over reversible electron transfer direct from the particle conduction band or shallow electron traps just below the conduction band edge. The oxidative current due to the latter effect exhibits a range of onset potentials arising from the polydisperse, Q-state nature of the particles under interrogation. The steady-state photoelectrochemistry varies from that in the dark in that (i) the surface states play a different role in determining the shape of the current voltage curve as they have been mostly oxidised by photogenerated valence band holes; and (ii) the photocurrent onset shifts to more anodic potentials as a result of a surface state-driven photocurrent attenuation and positive charge accumulation at the particle surface, both derived from hole-driven surface state oxidation. Light-on transient photocurrent measurements with the ORDE allow calculation of a pseudo-first-order rate coefficient for photogenerated electron loss, k(0), of similar to 0.07 s(-1). This suggests that the loss process being interrogated is not photogenerated electron-valence band hole recombination, but the loss of electrons left on the particle after some valence band hole filling reaction has occurred. Transient experiments also allow calculation of phi, the quantum efficiency for the photogeneration of electrons detectable by the ORDE. phi is found to be similar to 0.006, indicating that the dominant processes within the particle are direct and indirect photogenerated electron-valence band hole recombination.

AB - Results are presented for the dark and photoelectrochemistry of colloidal CdS particles studied with the optical rotating disc electrode (ORDE). The behaviour of the particles in the dark is governed by reversible electron transfer from a range of surface states superimposed over reversible electron transfer direct from the particle conduction band or shallow electron traps just below the conduction band edge. The oxidative current due to the latter effect exhibits a range of onset potentials arising from the polydisperse, Q-state nature of the particles under interrogation. The steady-state photoelectrochemistry varies from that in the dark in that (i) the surface states play a different role in determining the shape of the current voltage curve as they have been mostly oxidised by photogenerated valence band holes; and (ii) the photocurrent onset shifts to more anodic potentials as a result of a surface state-driven photocurrent attenuation and positive charge accumulation at the particle surface, both derived from hole-driven surface state oxidation. Light-on transient photocurrent measurements with the ORDE allow calculation of a pseudo-first-order rate coefficient for photogenerated electron loss, k(0), of similar to 0.07 s(-1). This suggests that the loss process being interrogated is not photogenerated electron-valence band hole recombination, but the loss of electrons left on the particle after some valence band hole filling reaction has occurred. Transient experiments also allow calculation of phi, the quantum efficiency for the photogeneration of electrons detectable by the ORDE. phi is found to be similar to 0.006, indicating that the dominant processes within the particle are direct and indirect photogenerated electron-valence band hole recombination.

KW - SMALL SEMICONDUCTOR PARTICLES

KW - CHARGE-TRANSFER PROCESSES

KW - LIQUID-SOLID INTERFACE

KW - CADMIUM-SULFIDE

KW - PHOTOREDOX REACTIONS

KW - RADIATION-CHEMISTRY

KW - TRAPPED ELECTRONS

KW - OXIDE COLLOIDS

KW - PHOTOCHEMISTRY

KW - FEMTOSECOND

U2 - 10.1039/B001338M

DO - 10.1039/B001338M

M3 - Journal article

VL - 2

SP - 3641

EP - 3650

JO - Physical Chemistry Chemical Physics

JF - Physical Chemistry Chemical Physics

SN - 1463-9076

IS - 16

ER -