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Illumination stepped

The key point of this discussion is that it shows that analysis of the transient photocurrent response allows separation of ktr and krec. The ratio /Pho.o(00)/yPho o(0) is given by kj(ktr + knc) and a plot of ln(/photo(0 - jpho. to(/infinity)) vs. t has a slope of -(ktr + krec). It is important to note that the analysis is only possible if recombination occurs. For krec— 0, the photocurrent simply follows the illumination step, and 4>(f) = 1. [Pg.240]

Fig. 8.6. Components of the current response of a n-type semiconductor electrode to an illumination step. ch is the charging current, is the current due to interfacial electron transfer and rc,. is the current due to electrons recombining with holes via surface states. The total current, given by the sum of and j , is equal to qg - /rec, where g is the flux of minority carriers given by the Gartner equation. The dimensionless normalised time axis is ( lr + k,c<.)t. The dimensionless normalised current axis is jlqg. Fig. 8.6. Components of the current response of a n-type semiconductor electrode to an illumination step. ch is the charging current, is the current due to interfacial electron transfer and rc,. is the current due to electrons recombining with holes via surface states. The total current, given by the sum of and j , is equal to qg - /rec, where g is the flux of minority carriers given by the Gartner equation. The dimensionless normalised time axis is ( lr + k,c<.)t. The dimensionless normalised current axis is jlqg.
Examination of equation (8.48) shows that the transient microwave response still contains information when there is no surface recombination. By contrast, if krcc = 0, the photocurrent simply follows the illumination step and contains no information about the rate of charge transfer at the interface. If krcc = 0, equation (8.48) becomes... [Pg.263]

From the DSC experiment, it is evident that the iron cation is less reactive in epoxide polymerization then Brensted acids obtained from, e.g. sulfonium salts (see Fig. 11). Therefore, a heat treatment after the illumination step is necessary. The narrow enthalpy peak observed could refer to a very uniform pathway. [Pg.71]

In this section, we briefly consider the response of nanocrystalline semiconductor-electrolyte interfaces to either pulsed or periodic photoexcitation. Several points are worthy of note in this respect (a) the photocurrent rise-time in response to an illumination step is nonlinear. Further, the response is faster when the light intensity is higher, (b) The decay profiles exhibit features on rather slow time-scales extending up to several seconds, (c) The photocurrent decay transients exhibit a peaking behavior. The time at which this peak occurs varies with the square of the film thickness, d. (d) A similar pattern is also seen in IMPS data where the transit time, r, is seen to be proportional to d. ... [Pg.2706]

Post-modification Reaction. After the illumination step, the substrate was immersed in a solution of 200 pL perfluorobutyryl chloride and 50 pL triethyl amine in 2 mL CH2C12 for 20 min. The substrates were washed with CH2C12 and dried in a stream of nitrogen. [Pg.110]

Fig. 30. Transient photocurrent response to illumination step measured at low light intensity for n-Si in 1.0 M NH4F at pH 4.5 [49]. The slow rise and fall are attributed to the slowest step in the photocurrent multiplication scheme. The semilogarithmic plot can be used to derive the value of k. Compare with Fig. 29 which demonstrates the superior resolution of IMPS. Fig. 30. Transient photocurrent response to illumination step measured at low light intensity for n-Si in 1.0 M NH4F at pH 4.5 [49]. The slow rise and fall are attributed to the slowest step in the photocurrent multiplication scheme. The semilogarithmic plot can be used to derive the value of k. Compare with Fig. 29 which demonstrates the superior resolution of IMPS.
It can be seen that the risetime of the photocurrent in response to the illumination step is much faster when the light intensity is higher (b). The rise in photocurrent clearly does not correspond to a simple first order process, as is shown by the nonlinear semilogarithmic plot of the photocurrent rise in Fig. 36. Marked non-linearity has also been observed in time of flight experiments of electron and hole transport in amorphous silicon [167]. [Pg.138]

Preliminary illumination steps leading to the formation of OH radicals TiOi + hv h + e ... [Pg.161]

The electrophotographic system (102,103) involves two key physicochemical elements a photoreceptor and a toner. The minimum requirements of the process are (/) to charge a photoconductive photoreceptor uniformly (2) to illuminate selectively the photoreceptor to form a latent electrostatic image and (J) to develop the image by applying charged toner. These steps are illustrated in Figure 17. [Pg.51]

A make-shift arrangement, it was not the most efficient system. Picatinny s pyrotechnics experts stepped into the picture. Within a matter of weeks, a new illuminating rifle grenade was developed and delivered to front line troops,... [Pg.748]

The lipase (PAL) used in these studies is a hydrolase having the usual catalytic triad composed of aspartate, histidine, and serine [42] (Figure 2.6). Stereoselectivity is determined in the first step, which involves the formation of the oxyanion. Unfortunately, X-ray structural characterization of the (S)- and (J )-selective mutants are not available. However, consideration of the crystal structure of the WT lipase [42] is in itself illuminating. Surprisingly, it turned out that many of the mutants have amino acid exchanges remote from the active site [8,22,40]. [Pg.33]

The deposition takes place from HTeOs and cadmium-EDTA complex solutions at a potential whereat, whilst Te is deposited from HTeOs under a diffusion-limited condition, the Cd-EDTA complex ion is not reduced to metallic Cd. The first step is the dark deposition of one monolayer of elemental Te on the p-Si substrate (Fig. 4.11a, i). After completion of this step, as specified by measuring the charge passed, the electrode is illuminated by light with energy higher than the band gap energy of silicon for a limited time. Then conduction band electrons are... [Pg.181]

When Munsell devised his color space, he did so on the basis of minimum observable color perception steps. But the problem with the Munsell System was one of reproducibility, which the CIE Standard Observer cured. In formulating a color match, one wants to be able to predict the correct concentration of colorants required, whose scattering and absorption properties are known, i.e.- the lightness, so as to match the sample submitted, starting with their spectrophotometric curves. In practice, this is not so simple, since two colors must have identical spectrophotometric curves to be exactly equal. It turns out that the human eye will identify the two colors to be equal if their spectrophotometric reflectances are reasonably close. Two colors may appear to be equal under Daylight illumination, but quite different under incandescent lamp illumination. These colors are known zus "metamers" and the phenomenon "metamerism". [Pg.435]

The efficiency of semiconductor PCs in some reactions (such as dehydrogenation of organics, splitting of HjO and H2S, etc.) can be enhanced by depositing tiny islands of additional catalysts, which facilitate certain reactions stages that may not require illumination. For example, islands of Pt metal are deposited on the surface of the composite photocatalyst in Fig.6 with the aim to facilitate the step of H2 formation. [Pg.44]

In our approach to membrane breakdown we have only taken preliminary steps. Among the phenomena still to be understood is the combined effect of electrical and mechanical stress. From the undulational point of view it is not clear how mechanical tension, which suppresses the undulations, can enhance the approach to membrane instability. Notice that pore formation models, where the release of mechanical and electrical energy is considered a driving force for the transition, provide a natural explanation for these effects [70]. The linear approach requires some modification to describe such phenomena. One suggestion is that membrane moduli should depend on both electrical and mechanical stress, which would cause an additional mode softening [111]. We hope that combining this effect with nonlocality will be illuminating. [Pg.94]


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See also in sourсe #XX -- [ Pg.309 , Pg.310 , Pg.311 , Pg.312 , Pg.313 , Pg.314 , Pg.315 ]




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Illuminated

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