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Positive-going feature

Time-resolved mid-IR spectra of several photolyzed heme proteins are shown in Fig. 6. The negative-going features correspond to loss of bound CO (A states) and the positive-going features correspond to CO dissociated from the heme (B states). Note the transition frequencies and relative intensities of the A and B states. When CO is bound to heme, back-bonding between the CO -orbitals and the iron d-orbitals weakens the CO bond and enhances its transition moment (42). Compared to free CO, the bound CO vibrational frequency is red shifted about 200 cm 1 and its integrated oscillator strength at 5.5 K is enhanced 21.7 1.6 times (33). [Pg.223]

We showed in the preceding section that for solids with strong vibrational bands the position of features in absorption spectra can be shifted appreciably in going from the bulk to particulate states. Metallic particles can deviate even more markedly from the behavior of the bulk parent material they can have absorption features over broad frequency regions where none appear in the bulk. For a simple metal—one that is well described by the Drude formula... [Pg.335]

At room temperature, the cyclic voltammogram features an irreversible two-electron reduction (peak a) with oxidation of the monomeric anion evident on the return sweep (peak b). As the temperature is lowered, a new peak (peak c) grows in on the positive-going scan. This peak, due to oxidation of the dimeric radical anion to starting material, grows at the expense of peak b until the latter is entirely absent at -76°C. These results are qualitatively in accord with... [Pg.492]

Figure 6b also reveals that the positive lobe of the bipolar band around 1280 cm decreases at potentials above 0.45 V this decline coincides with the onset of the surface oxidation in the voltammetry of Ru(OOOl) (c.f., Fig. 2). Adsorption of the OH species is followed by the desorption of bisulfate and a concurrent increase in the bisulfate species in the double layer. This effect becomes visible in the IR spectrum by the appearance of the positive-going solution-phase bands for the bisulfate anion at 1051 and 1200 cm at potentials equal to, or higher than 0.55 V. The most pronounced feature in the IR spectra above 0.55 V is the negative lobe of the bipolar band centered at 1248 cm , which represents adsorbed bisulfate at the reference potential. Figure 6b also reveals that the positive lobe of the bipolar band around 1280 cm decreases at potentials above 0.45 V this decline coincides with the onset of the surface oxidation in the voltammetry of Ru(OOOl) (c.f., Fig. 2). Adsorption of the OH species is followed by the desorption of bisulfate and a concurrent increase in the bisulfate species in the double layer. This effect becomes visible in the IR spectrum by the appearance of the positive-going solution-phase bands for the bisulfate anion at 1051 and 1200 cm at potentials equal to, or higher than 0.55 V. The most pronounced feature in the IR spectra above 0.55 V is the negative lobe of the bipolar band centered at 1248 cm , which represents adsorbed bisulfate at the reference potential.
Figure 8.1 Ultrafast transient absorption dynamics, (a) Positive-going signal is the absorption of charge carriers which is affected by the amount of solvent additive (DIO). Negative-going features are the photobleaching signals of the neutral donor molecule, and are unaffected by solvent additives, (b) Qualitative charge transfer timescales obtained by fitting the traces of panel (a) with a model which accounts for a pulse width of 100 fs. Reproduced from ref. 10. Copyright 2012 American Chemical Society. Figure 8.1 Ultrafast transient absorption dynamics, (a) Positive-going signal is the absorption of charge carriers which is affected by the amount of solvent additive (DIO). Negative-going features are the photobleaching signals of the neutral donor molecule, and are unaffected by solvent additives, (b) Qualitative charge transfer timescales obtained by fitting the traces of panel (a) with a model which accounts for a pulse width of 100 fs. Reproduced from ref. 10. Copyright 2012 American Chemical Society.
Continuum models go one step frirtlier and drop the notion of particles altogether. Two classes of models shall be discussed field theoretical models that describe the equilibrium properties in temis of spatially varying fields of mesoscopic quantities (e.g., density or composition of a mixture) and effective interface models that describe the state of the system only in temis of the position of mterfaces. Sometimes these models can be derived from a mesoscopic model (e.g., the Edwards Hamiltonian for polymeric systems) but often the Hamiltonians are based on general symmetry considerations (e.g., Landau-Ginzburg models). These models are well suited to examine the generic universal features of mesoscopic behaviour. [Pg.2363]

SOMe the enhancement in the meta-position is almost as large as in the para-position. The authors go on to show the applicability of op (g) values to certain solution processes, particularly those in non-aqueous solvents, but including the dissociation of thiophenols in 48% ethanol, the results of Bordwell and Andersen80 to which reference has been made earlier (Section III.A.1). A separation of field/inductive and resonance effects is also essayed for the gas-phase acidities of the phenols, and SOMe and S02Me feature in the discussion. There is reference to a oR° value of + 0.07 for SOMe as an unpublished result of Adcock, Bromilow and Taft (cf. 0.00 from Ehrenson and coworkers65 and — 0.07 from Katritzky, Topsom and colleagues128.)... [Pg.517]


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See also in sourсe #XX -- [ Pg.436 ]




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