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Absorption spectra collections

Figure 1 shows absorption spectra collected at different times after mixing AuCU" ions with neutralized PEG 20M (pH = 5.5). Similar results were obtained using HNO3 or HCl to neutralize the polymer samples. For times shorter than 15 min, the plasmon... [Pg.129]

The DSC cell is placed on the stage of an infi ared microscope. As the material is being heated, and while the DSC curve is being generated, infirared spectra are continually collected by micro-reflection/absorption. Spectra collected during a thermal transition may be compared and interpreted to explain, on a molecular level, the cause of this transition. [Pg.150]

The EXAFS modulations in E space, x(E), where E is the absolute energy of the X-rays, are defiend as [(jlIE) - /u.o( )]//u.o( ) or AiJi,(E)liJiQ(E), where fi(E) is the normalized absorption cross section of the element in the compound of interest and /ji.q(E) is the absorption coefficient of an isolated atom. The X-ray absorption spectrum collected using the normal detection methods employed (described above) does not measure the absolute cross section, but only the relative cross section. Therefore, it is necessary to normalize all EXAFS spectra to unit edge height at a particular energy E (position of the edge maximum is a common choice). [Pg.660]

Let us come back to the sample preparation A drop of solution containing silver nanoparticles dispersed in hexane is deposited on the substrate. The nanocrystals can be removed by washing the substrate and collected in hexane. The absorption spectrum of silver particles recorded before and after deposition remains the same. This indicates that coalescence does not take place. Similar behavior was observed by using HOPG as a substrate [6,35]. [Pg.327]

On this basis = 0.0170 sec , = 0.645 sec , and K = 0.739 mole.P at 25 °C. The corresponding activation parameters were determined also by Es-penson. By a method involving extrapolation of the first-order rate plots at various wavelengths to zero time, the absorption spectrum of the intermediate was revealed (Fig. 1). Furthermore, the value of K obtained from the kinetics was compatible with that derived from measurements on the acid dependence of the spectrum of the intermediate. Rate data for a number of binuclear intermediates are collected in Table 2. Espenson shows there to be a correlation between the rate of decomposition of the dimer and the substitution lability of the more labile metal ion component. The latter is assessed in terms of the rate of substitution of SCN in the hydration sphere of the more labile hydrated metal ion. [Pg.158]

For several technical reasons, it is not possible to acquire NMR data with perfect phase. One reason is the inability to detect XY magnetisation correctly another is the fact that we are unable to collect the data as soon as the spins are excited. These limitations mean that we have to phase correct our spectrum so that we end up with a pure absorption spectrum. What we don t want is a dispersion signal (see Spectrum 4.2). [Pg.36]

Light-harvesting molecules on a planet around a local star have developed an absorption spectrum to collect light at the maximum flux from the local star... [Pg.38]

In the diffuse reflectance mode, samples can be measured as loose powders, with the advantages that not only is the tedious preparation of wafers unnecessary but also diffusion limitations associated with tightly pressed samples are avoided. Diffuse reflectance is also the indicated technique for strongly scattering or absorbing particles. The often-used acronyms DRIFT or DRIFTS stand for diffuse reflectance infrared Fourier transform spectroscopy. The diffusely scattered radiation is collected by an ellipsoidal mirror and focussed on the detector. The infrared absorption spectrum is described the Kubelka-Munk function ... [Pg.224]

The sunlight is absorbed by a number of pigments, of which chlorophyll a is the most important. The absorption spectrum of chlorophyll a is shown in Fig. 10.3. Apart from chlorophyll a there are accessory pigments which function as lightharvesting antennae and transfer the energy to the chlorophyll a. This is an elegant way to efficiently collect sunlight. [Pg.340]

The XANES region of the Pt Lm and Ln absorption edges can be used to determine the fractional d-electron occupancy of the Pt atoms in the catalyst sample by a so-called white line analysis. Figure 2 shows the XAS spectrum collected at both Pt Lm and Lii absorption edges of Na2Pt(OH)e. The sharp features at the absorption edges are called white lines after the white line observed in early photographic film based XAS measurements. Mansour and coworkers have shown that comparison of the white line intensities of a sample with those of a reference metal foil provides a measure of the fractional d-electron vacancy, f, of the absorber atoms in the sample. is defined as follows ... [Pg.376]

One often unsuspected source of error can arise from interference by the substances originating in the sample which are present in addition to the analyte, and which are collectively termed the matrix. The matrix components could enhance, diminish or have no effect on the measured reading, when present within the normal range of concentrations. Atomic absorption spectrophotometry is particularly susceptible to this type of interference, especially with electrothermal atomization. Flame AAS may also be affected by the flame emission or absorption spectrum, even using ac modulated hollow cathode lamp emission and detection (Faithfull, 1971b, 1975). [Pg.204]

The lack of a clearly developed peak in the UV-visible absorption spectrum due to plasma resonance places a limit on the collective metallic behavior of the electrons in the cluster. On the other hand, the 5d -y 6s,6p interband absorption is well developed toward that of large colloidal gold particles. [Pg.35]

Such a process would have an intensity exponent of unity as observed. A further fact in support of the disproportionation mechanism is that the yield of CF2CI2 is largely independent of the ketone pressure at room temperature an abstraction mechanism would require a first-order dependence upon ketone pressure. While the dimer of CF2, tetrafluoro-ethylene, has never been observed in the reaction mixture, a white solid collected in the cell which was probably a polymer of CF2. While the experimental conditions are not strictly comparable, it is significant that the absorption spectrum of CF2 has been observed in the flash photolysis of 1,3-dichlorotetrafluoroacetone.39 When the temperature is raised, however, the yield of CF2C12 in normal photolysis, increases rapidly suggesting an energy of activation and this process can only be chlorine abstraction. The rate function ... [Pg.172]

Studies utilizing these characterization techniques to identify the bonding state of both carbon and nitrogen atoms in C-N thin films include XPS [59], EELS [60], RS [61], and FT-IR absorption spectrum [62,63]. These studies have collectively demonstrated the existence of various chemical bonding states such as C-N, C = N, and C=N, indicating that a C-N film is not a pure homogeneous phase. [Pg.772]

Baylor et. al. have provided recent in-vitro isotropic absorption spectrum for Rhodonine based on Macaca fascicularis143. The data was collected over five and one-half orders of intensityusing transverse illumination at near 37 Celsius. Baylor, et. al. also provide a review of other available measurements and perform a circuitous calculation to compare the isotropic spectrum to the human scotopic luminous efficiency function attributed to Carpenter rather than the C.I.E. Based on ten photoreceptors, the peak sensitivity was estimated to be 491 nm. This is lower than most other investigators. However, data points were only collected at 20 nm intervals using filters of 10 nm nominal half-widths. This sampling plan does not support three digit accuracy in their peak value. [Pg.87]


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See also in sourсe #XX -- [ Pg.788 , Pg.817 ]




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Spectra, collections

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