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Differential reflectance studies

A typical experimental set-up for differential reflectance is shown in Fig. 112. To ensure that slow variations in the power of the lamp are adequately monitored, a rotating silvered chopper is used that either reflects the light [Pg.240]

An example of the use of the technique to obtain information during a cyclic voltammagram is shown in Fig. 113 for n-ZnO [192], As the crystal was cycled to very negative potentials, a large cathodic current was found due both to hydrogen evolution and Zn-metal deposition from the reductive decomposition of the ZnO. Re-oxidation of the Zn metal is seen as an anodic peak in the CV, but it is very difficult, in the presence of both cathodic and anodic currents, to form a clear impression from the CV of the amount of Zn [Pg.241]

Goodenough and A. Hamnett, in 0. Madelung (Ed.), Non-tetrahedrally Bonded Semiconductors, Landolt-Bornstein Neue Serie Vol. XVII/g, Springer-Verlag, Berlin, 1984. [Pg.242]

Semiconductors, Cambridge University Press, London, 1979. [Pg.242]

Kittel, Introduction to Solid State Physics, Wiley, New York, 6th edn., 1986. [Pg.242]


The initial stages, notably the formation of a monolayer on a foreign substrate at underpotentials, were mainly studied by classical electrochemical techniques, such as cyclic voltammetry [8, 9], potential-step experiments or impedance spectroscopy [10], and by optical spectroscopies, e.g., by differential reflectance [11-13] or electroreflectance [14] spectroscopy, in an attempt to evaluate the optical and electronic properties of thin metal overlayers as function of their thickness. Competently written reviews on the classic approach to metal deposition, which laid the basis of our present understanding and which still is indispensable for a thorough investigation of plating processes, are found in the literature [15-17]. [Pg.108]

Seliga, T. A., V. N. Bringi, and H. H. Al-Khatib, 1981. A preliminary study of comparative measurements of rainfall rate using the differential reflectivity technique and a raingauge network,./ Appl. Meteorol., 20. 1362- 1368. [Pg.515]

The following papers focus mainly on various aspects associated with the self-assembly of peptides. Peptides are relatively short sequences of amino acids, typically less than 50. The limited number of residues brings simplicity but still allows for sufficient differentiation to study self-assembly in its various details. The compositional freedom of the primary molecule allows for a sufficiently rich hierarchical structure creation through aggregation of individual peptides into supramolecular constructs resulting in interesting materials. This chapter looks into relevant patent literature as a reflection of the state of the art of technology in peptide self-assembly. [Pg.2]

The structures were grown in an ultra high vacuum (UHV) chamber VARIAN with a base pressure of 2-10 °Torr equipped with differential reflectance spectroscopy (DRS) [3] for a study of optical properties of the samples. Samples were cut from n-type 0.3 D cm Si(l 11) substrates. The silicon was cleaned by flashes at 1250 °C (7 times). Surface purity was controlled by AES. RDE was carried out at 500 °C, 550 °C, and 600 °C. The Cr deposition rate was about 0.04 nm/min controlled by a quartz sensor. An additional annealing during 2 min at 700 °C was done for all samples before the growth of silicon epitaxial cap layer. [Pg.96]

Growth experiments were carried out in two ultra high vacuum (UHV) cambers with sublimation sources of Si, Fe and Cr and quartz sensors of film thickness. Optical properties of the samples were studied in UHV chamber VARIAN (210 10Torr) equipped with differential reflectance spectroscopy (DRS) facilities. The samples surface was studied in the second UHV chamber (1 -10 9 Torr) equipped with LEED optics. Si(100) and Si(l 11) wafers were used as substrates for different series of the growth experiments. For the growth of silicide islands, metal films of 0.01-1.0 nm were deposited onto silicon surface. Silicon overgrowth with the deposition rate of 3-4 nm/min was carried out by molecular beam epitaxy (MBE) at 600-800 °C for different substrates. The samples were then analyzed in situ by LEED and ex situ by HRTEM and by... [Pg.176]

Case 1. The first case arises because a PCA model is based on describing data variance as a consequence, the variables showing large variation are implicitly important, that is, more important than the others. The point is, why do those variables have a bigger variability In case the variation is solely due to a matter of scale (units of measure) or if it reflects the different amount of compounds (the presence of major and minor constituents albeit all potentially interesting to describe/differentiate the studied samples), it is fair to scale variables. On the contrary, if the variation is only due to noise... [Pg.97]

In a systematic study, the deposition of thin Ag overlayers on a Cu(lll) electrode was investigated by electroreflectance and differential reflectance spectroscopy, employing an optical thin-layer cell (Figure Figure 55... [Pg.172]

We now return to the question about the role of nonlocal optics in the study of metal electrodes. In Figure 56a, the differential reflection spectra are shown for a Cu(lll) electrode covered with a thin Ag overlayer i.e., R/R represents the reflectance change of the Cu(lll) electrode due to deposition of a 5-monolayer-thick Ag These experimental spectra can then be... [Pg.173]

K. and Enyo, M. (1989) Surface species produced on Pt electrodes during HCHO oxidation in sulfuric add solution as studied by infrared reflection-absorption spectroscopy (IRRAS) and differential electrochemical mass spectroscopy (OEMS)./. Electroanal. Chem., 258, 219-225. [Pg.101]


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