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Charge transfer symmetric

Figure 11. Photoion photoelectron coincidence studies of charge-transfer reactions of state-selected ions. Cross sections for nitric oxide symmetric charge-transfer reaction are plotted as function of reactant-ion kinetic energy and reactant-ion vibrational state (o = 0,1,2,3,4,5). Solid lines are linear least-squares fits to experimental data (not shown).86c... Figure 11. Photoion photoelectron coincidence studies of charge-transfer reactions of state-selected ions. Cross sections for nitric oxide symmetric charge-transfer reaction are plotted as function of reactant-ion kinetic energy and reactant-ion vibrational state (o = 0,1,2,3,4,5). Solid lines are linear least-squares fits to experimental data (not shown).86c...
The products of reactive ion-neutral collisions may be formed in a variety of excited states. Excited products from nonreactive collisions have already been discussed in a previous section. Theoretical calculations of vibrational excitation in the products of symmetric charge-transfer reactions have also been mentioned previously.312-314 The present section deals with excited products from reactive ion-neutral scattering, with special emphasis on luminescence measurements. [Pg.163]

A symmetric charge transfer and a change of the quadrupole moment appear to be important. [Pg.178]

Fig. 2. The use of a de ejection field within the collision chamber to extract product ions formed with a thermal energy distribution. Here, the product ions are argon ions formed by symmetric charge transfer from a 60-eV argon primary ion beam (laboratory energy). The argon product ion intensity (in arbitrary units) is plotted as a function of the potential (in volts) applied to the exit slit with respect to the entrance slit. The collision chamber is 0.5 cm long. A constant, residual argon ion intensity is to be noticed at negative potentials these are product ions formed from reaction outside the collision chamber. Fig. 2. The use of a de ejection field within the collision chamber to extract product ions formed with a thermal energy distribution. Here, the product ions are argon ions formed by symmetric charge transfer from a 60-eV argon primary ion beam (laboratory energy). The argon product ion intensity (in arbitrary units) is plotted as a function of the potential (in volts) applied to the exit slit with respect to the entrance slit. The collision chamber is 0.5 cm long. A constant, residual argon ion intensity is to be noticed at negative potentials these are product ions formed from reaction outside the collision chamber.
This includes the symmetric charge-transfer channel. [Pg.175]

CHj (via several mechanisms), CH4 (via symmetric charge transfer), or CHj (via collision-induced dissociation of CH4 or fragmentation of the excited CH5 product). [Pg.177]

Fig. 19. Comparison of experimental data for the symmetric charge-transfer reaction Ar (Ar,Ar)Ar at low energy. The sources of the data are as indicated Ziegler/ Cramer/ Nichols and Witteborn, Neynaber et Birkinshaw, and... Fig. 19. Comparison of experimental data for the symmetric charge-transfer reaction Ar (Ar,Ar)Ar at low energy. The sources of the data are as indicated Ziegler/ Cramer/ Nichols and Witteborn, Neynaber et Birkinshaw, and...
Related to this type of approach, but conceptually distinct, is the use of the two-state model, familiar in its application to symmetric charge-transfer reactions. Implicit in the model is the idea that the transition between the initial reactant and final product states may occur at large reactant separations. Bohme have extended this model to consider... [Pg.223]

A year ago, one could say with some confidence that the excitation functions of these symmetric charge-transfer reactions were some of the most reliably established (p. 183), to the point that the argon reaction was suggested as a calibrating standard in Section 5.2.1. Today there is considerable uncertainty which hopefully will receive attention and resolution. [Pg.242]

The three-photon transition amplitude has been shown to be obtainable from the single residue of the appropriate CRF [27], although the technique has been employed only rarely. Lin et al. [247] analyzed for instance, solvent effects (accounted for by PCM) on the three-photon absorption spectrum of a symmetric charge transfer molecule using TD-DFT. [Pg.115]

For a special case of a = p, a case of symmetric charge transfer coefficient for anodic and cathodic reactions. Equation 5.77 becomes... [Pg.185]

To appreciate this step, it will be useful to consider earlier developments in asymmetric and symmetric charge transfer. There have been a number of relatively recent reviews in these areas (Basu et al., 1978 Belkic et al., 1979 Shakeshaft and Spruch, 1979 Shakeshaft, 1982), and we limit ourselves to some brief comments. [Pg.410]


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See also in sourсe #XX -- [ Pg.422 ]




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