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Counter-illumination

Quantum counter Illumination excites electron to a higher level, a pump signal excites it to an even higher level. The electron is finally de-excited with an emission of photon detected by a separate detector. Noise of these devices is negligible, but their sensitivity is low... [Pg.10]

The photoelectrolysis of H2O can be performed in cells being very similar to those applied for the production of electricity. They differ only insofar as no additional redox couple is used in a photoelectrolysis cell. The energy scheme of corresponding systems, semiconductor/liquid/Pt, is illustrated in Fig. 9, the upper scheme for an n-type, the lower for a p-type electrode. In the case of an n-type electrode the hole created by light excitation must react with H2O resulting in 02-formation whereas at the counter electrode H2 is produced. The electrolyte can be described by two redox potentials, E°(H20/H2) and E (H20/02) which differ by 1.23 eV. At equilibrium (left side of Fig. 9) the electrochemical potential (Fermi level) is constant in the whole system and it occurs in the electrolyte somewhere between the two standard energies E°(H20/H2) and E°(H20/02). The exact position depends on the relative concentrations of H2 and O2. Illuminating the n-type electrode the electrons are driven toward the bulk of the semiconductor and reach the counter electrode via the external circuit at which they are consumed for Hj-evolution whereas the holes are dir tly... [Pg.97]

The apparatus used for studying the photoelectrochemical behavior (11) of the Ti02 film electrode is shown in Figure 5- Platinum plate of 35x25 mm and saturated calomel electrode (S.C.E.) were employed as a counter and a reference electrode, respectively. A 500 W Xenon lamp was used for illuminating the Ti02 electrode. [Pg.350]

A representative example of the upd process is copper on gold and an extremely illuminating study of this system using repulsive AFM was reported by Manne et al. (1991). The authors employed a commercially available AFM, the essentials of which are shown in Figure 2.33. The reference electrode was a copper wire in contact with the electrolyte at the outlet of the cell. The counter electrode was the stainless steel spring clip holding the AFM cantilever in place. The working electrode was a 100 nm thick evaporated Au film (which is known to expose mainly the Au(111) surface) mounted on an (x, v) translator. [Pg.92]

Figure 11.8 Schematic diagrams of the Fujishima-Honda cell using an illuminated Ti02 (rutile) semiconductor electrode and a platinum counter-electrode... Figure 11.8 Schematic diagrams of the Fujishima-Honda cell using an illuminated Ti02 (rutile) semiconductor electrode and a platinum counter-electrode...
DISABLE COUNTERS The disabling of the counters causes the excitation to be turned off. The sample is not illuminated when data are not collected. In this manner, problems that arise due to long exposures of the sample and reference to excitation (bleaching and heating) are minimized. [Pg.287]

Figure 2. Cell and circuit used in experiments like those in Figure 1. (1) Illuminated TiOg electrode (2) platinum counter electrode in the Sark (3) reference electrode (SCE) (4) buffered electrolyte solution (5) quartz window for UV light (A) ammeter (V) voltmeter (11). Figure 2. Cell and circuit used in experiments like those in Figure 1. (1) Illuminated TiOg electrode (2) platinum counter electrode in the Sark (3) reference electrode (SCE) (4) buffered electrolyte solution (5) quartz window for UV light (A) ammeter (V) voltmeter (11).
Equipment PCR machine, scintillation counter, tabletop centrifuge, temperature-controlled water baths, equipment for horizontal and vertical electrophoresis, UV-illuminator, phosphor imager, automatic DNA sequencer, vacuum dot-blot manifold (Schleicher and Schuell). PCR 0.5 ml hot-start mbes, aerosol resistant pipette rips, autoclaved Eppendorf tubes (all from Fischer Scientific, Brightwaters, NY) and glassware, diethyl pyrocarbonate (DEPC, Sigma)-treated solutions. [Pg.22]

Fig. 3.23 Efficiency under near UV illumination of a photoelectrochemical cell comprised of a titania nanotube array photoanode and Pt counter electrode. For the calculation of efficiency using equation (3.6.13), a two electrode geometry was used while for the calculation using equations (3.6.15a) and (3.6.16), a three electrode geometry was used. Fig. 3.23 Efficiency under near UV illumination of a photoelectrochemical cell comprised of a titania nanotube array photoanode and Pt counter electrode. For the calculation of efficiency using equation (3.6.13), a two electrode geometry was used while for the calculation using equations (3.6.15a) and (3.6.16), a three electrode geometry was used.
Ip is the photocurrent density in mA cm, AE the potential difference between working electrode and counter electrode under illumination minus the potential difference between the same electrodes without illumination (dark). That is, AE is the photovoltage with dark voltage subtracted from it. This equation is misleading and has no thermodynamics basis. AE does not necessarily represent the sample behavior but it depends upon the experimental conditions. Furthermore the hydrogen produced at current Ip can yield a power output higher than Ip AE. [Pg.174]

Like other non-oxidic semiconductors in aqueous solutions, surface oxidized and photocorrosive InP is a poor photoelectrode for water decomposition [19,27,32,33], To enhance properties several efforts have focused on coupling of the semiconductor with discontinuous noble metal layers of island-like topology. For example, rhodium, ruthenium and platinum thin films, less than 10 nm in thickness, have been electrodeposited onto p-type InP followed by a brief etching treatment to achieve an island-like topology on the surface [27,28]. In combination with a Pt counter electrode, under AM 1.5 illumination of 87 mW/cm the metal (Pt, Rh, Ru) functionalized p-InP photocathodes [27] see a reduction in the threshold voltage for water electrolysis from 1.23 V to 0.64 V, and in aqueous HCl solution a photocurrent density of 24 mA/cm with a photoconversion efficiency of 12% [27]. [Pg.451]

Photoelectrochemical effect involves production of a voltage and an electric current when light falls on a semiconductor electrode immersed in an electrolyte solution and connected to a counter electrode (Becquerel, 1839). Working with germanium electrodes, Brattain Garrett (1955) showed that the Becquerel effect was due to the formation of a semiconductor-electrolyte junction. The idea of using an illuminated... [Pg.416]

Photocatalytic oxidation over illuminated titanium dioxide has been demonstrated to be effective at removing low concentrations of a variety of hazardous aromatic contaminants from air at ambient temperatures. At low contaminant concentration levels and modest humidity levels, complete or nearly complete oxidation of aromatic contaminants can be obtained in photocatalytic systems. Although aromatic contaminants are less reactive than many other potential air pollutants, and apparent catalyst deactivation may occur in simations where recalcitrant reaction intermediates build up on the catalyst surface, several approaches have already been developed to counter these potential problems. The introduction of a chlorine source, either in the form of a reactive chloro-olefin cofeed or an HCl-pretreated catalyst, has been demonstrated to promote the photocatalytic oxidation of... [Pg.279]

Fig. 2.1 Schematic representation of photoelectrochemical water electrolysis using an illuminated oxide semiconductor electrode. Open circuit (or small current), pH 2, illuminated conditions are shown for an oxide with an EcB of-0.65 V (SHE) and an Vb of 2.35 V (SHE). With an open circuit, a small excess potential ( 0.15 V) is available for H2 evolution, assuming a reversible counter electrode. Fig. 2.1 Schematic representation of photoelectrochemical water electrolysis using an illuminated oxide semiconductor electrode. Open circuit (or small current), pH 2, illuminated conditions are shown for an oxide with an EcB of-0.65 V (SHE) and an Vb of 2.35 V (SHE). With an open circuit, a small excess potential ( 0.15 V) is available for H2 evolution, assuming a reversible counter electrode.
As indicated in Figure 1, if a semiconductor is biased to depletion in contact with an electrolyte, a photocurrent can be generated upon illumination. This occurs because the photo-excited majority carriers are driven by the electric field in the depletion layer to the counter electrode and minority carriers migrate to the interface where they are trapped at the band edge. Nozik has recently speculated that hot minority carrier injection may play a role in supra-band edge reactions.(19)... [Pg.87]


See other pages where Counter-illumination is mentioned: [Pg.213]    [Pg.213]    [Pg.2132]    [Pg.207]    [Pg.271]    [Pg.102]    [Pg.245]    [Pg.226]    [Pg.21]    [Pg.217]    [Pg.461]    [Pg.467]    [Pg.494]    [Pg.494]    [Pg.325]    [Pg.120]    [Pg.155]    [Pg.165]    [Pg.171]    [Pg.447]    [Pg.448]    [Pg.449]    [Pg.502]    [Pg.30]    [Pg.417]    [Pg.574]    [Pg.93]    [Pg.223]    [Pg.31]    [Pg.279]    [Pg.370]    [Pg.46]    [Pg.256]    [Pg.71]    [Pg.117]    [Pg.86]   
See also in sourсe #XX -- [ Pg.213 ]




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