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Site-energy shift

The coordinates of all atoms were recorded every 2 fs, and were used to construct the time-dependent CC Hamiltonian including the solvent-induced site energy shifts. A typical MD simulation time was 1 ns for each trajectory. Fig. 6 shows snapshots of P4 along a 1 ns MD run with various positions of the single chromophores to each other. Compared with our earlier simulations reported in Ref. [8] the change from a methanol to an ethanol solvent reduced somewhat the conformational flexibility of P4. [Pg.56]

Figure 9.11 Promoter-induced binding energy shifts of Ar, Kr and Xe photoemission peaks with respect to adsorption on the clean metal as a function of the distance of the adsorption site to the nearest potassium atom on a potassium-promoted Rh( 111) surface. These curves reflect the variation of the surface potential (or local work function) around an adsorbed potassium atom. Note the strong and distance-dependent local work function at short distances and the constant local work function, which is lower than that of clean Rh( 111) at larger distances from potassium. The lowering at larger distances depends on the potassium coverage. The averaged distances between the potassium atoms are 1.61, 1.32 and 1.20 nm for coverages of 2.7, 4.1 and 5.0% respectively, vertical lines mark the half-way distances. Lines are drawn as a guide to the eye (adapted from Janssens et al. [38]). Figure 9.11 Promoter-induced binding energy shifts of Ar, Kr and Xe photoemission peaks with respect to adsorption on the clean metal as a function of the distance of the adsorption site to the nearest potassium atom on a potassium-promoted Rh( 111) surface. These curves reflect the variation of the surface potential (or local work function) around an adsorbed potassium atom. Note the strong and distance-dependent local work function at short distances and the constant local work function, which is lower than that of clean Rh( 111) at larger distances from potassium. The lowering at larger distances depends on the potassium coverage. The averaged distances between the potassium atoms are 1.61, 1.32 and 1.20 nm for coverages of 2.7, 4.1 and 5.0% respectively, vertical lines mark the half-way distances. Lines are drawn as a guide to the eye (adapted from Janssens et al. [38]).
We now investigate a model of the chemisorbed system, consisting of a semi-infinite DBA and a hydrogen-like adatom, as depicted in Fig. 6.2. The adatom, with initial electronic site energy ea, is attached to the surface atom (at site n = 1) by a bond of energy 7. Using the HF approximation to the ANG model ( 4.3), the effective adatom level of spin a is shifted to (4.34)... [Pg.103]

The second contribution on the right-hand side is the shift in the on site energy due to the neighbouring atomic potentials. In the spirit of our earlier treatment of diatomic molecules we will neglect this crystal field term. It does not fundamentally alter the band structure of either transition metals or semiconductors. The band structure, E(k), can, therefore, be written within the approximation as... [Pg.174]

Elongation Step 3 Translocation In the final step of the elongation cycle, translocation, the ribosome moves one codon toward the 3 end of the mRNA (Fig. 27-25a). This movement shifts the anticodon of the dipeptidyl-tRNA, which is still attached to the second codon of the mRNA, from the A site to the P site, and shifts the de-acylated tRNA from the P site to the E site, from where the tRNA is released into the cytosol. The third codon of the mRNA now lies in the A site and the second codon in the P site. Movement of the ribosome along the mRNA requires EF-G (also known as translocase) and the energy provided by hydrolysis of another molecule of GTP. [Pg.1060]

In Table 2 we summarize the results of the DDCI calculations on the lowest excitation energies for terrace, step and comer F and F+ centers. As expected, for a given transition the excitation energy decreases as the coordination of the defect decreases. For F centers, the allowed singlet to singlet lowest transition occurs at 3.4 eV for the surface, 2.9 eV for the step and 2.6 eV for the comer. The same trend is found for the F+ centers, where the first doublet to doublet transition, goes from 3.6 eV for the surface, to 2.6 eV for the step and 2.4 eV for the comer. As observed previously for the bulk calculations, excitations for the F+ centers appear around 0.2 eV below the excitations due to F centers. The excitations at the step and comer sites are shifted about 0.5-1.2 eV compared to... [Pg.236]

Fig. 9.n Promoter-induced binding energy shifts of Ar, Kr and Xe photoemission peaks with respect to adsorption on the clean metal as a function of the distance of the adsorption site to the nearest potassium atom on a potassium-promoted Rh(lll) surface. These curves reflect the variation of the surface potential (or local work function) around an adsorbed potassium atom. Note the strong and distance-dependent local work function... [Pg.268]

Here the 7 s are core-valence electron interaction terms, of which more will be said later, and nj is the number of valence electrons /. The first term gives the energy shift produced by chemical effects on the parent atom and the second refers to charge changes on the other lattice sites associated with the flow of charge... [Pg.99]

This approach was used to examine the redox chemistry of the Cu site in galactose oxidase (41), which had been proposed to contain an unusual Cu(III) center (52). The lack of a significant Cu K-edge energy shift between the oxidized and reduced forms of the protein demonstrated that the redox chemistry was not metal-centered and implicated another redox active site. The crystal structure of the protein subsequently revealed a novel thioether composed of a cysteine and a tyro-sinate ligand of the Cu site that is likely to be involved in the redox process (53). [Pg.37]


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Energy shifts

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