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Surface states charge transfer

Finally, some experimental observations are discussed in which charge transfer to surface states is important. The emphasis is on methods to be quantitative in describing the role of surface states by determining their density and reaction cross sections. Some previously published observations as well as preliminary new results are used to illustrate the role of surface bound species as charge transfer surface states. [Pg.105]

The effect of the FC term on ICT and MLCT-based chemosensors appears when the electron transfer rate constant is generalized within the context of nonradiative decay theory [191-193], MLCT excited states are produced directly upon excitation whereas ICT states are produced by a surface crossing from an initially prepared localized excited state (see Fig. 9). Return of the system from the charge transfer excited state to ground state has the overall form of an electron transfer recombination problem that is described by the inverted Marcus curve of Fig. 13. As described by the FC term of Eq. (5), the rate constant for... [Pg.20]

Fig. 10 The three-dimensional potential energy surface describing the motion of protons between N6(A) and 04(T) and between N3(T) and N1(A) shows two critical points in the ground state. The deeper minimum corresponds to the amine/keto structure of AT and a shallow one to the imine/enol structure (A T ). Upon absorption of a UV photon the initaly delocalized excitonic states (1) undergo a rapid localization on f 10 ps timescale for single bases and 100 ps timescale for stacked base pairs to form a charge transfer (CT) states. The subsequent CT states passing through a conical intersection are carried back to the ground state. Fig. 10 The three-dimensional potential energy surface describing the motion of protons between N6(A) and 04(T) and between N3(T) and N1(A) shows two critical points in the ground state. The deeper minimum corresponds to the amine/keto structure of AT and a shallow one to the imine/enol structure (A T ). Upon absorption of a UV photon the initaly delocalized excitonic states (1) undergo a rapid localization on f 10 ps timescale for single bases and 100 ps timescale for stacked base pairs to form a charge transfer (CT) states. The subsequent CT states passing through a conical intersection are carried back to the ground state.
Figure 60 also show s the Stcrn-Volmer plots for the quenching of the photoluminescence intensity. There is good agreement between the Stern-Volmer plots for the photoluminescence intensity and the yields of the photocatalytic isomerization reactions, indicating that both the photocatalytic reaction and the photoluminescence proceed through the same excited state of MgO, i.e., the charge-transfer excited state on the four-coordinated surface sites on MgO (96-98, 240). [Pg.230]

The factors which lead to the formation of an electrical double layer are rather general. First, charges flow across the interface when a thermodynamic equilibrium is established between the phases in contact second, it is charging processes, which are not generally related to charge transfer across the interface—for example, charging of surface states (see below), certain types of adsorption, etc. [Pg.201]

S. Chapman, The classical trajectory-surface-hopping approach to charge-transfer processes, State-Selected and State-to-State, Ion-Molecule Reaction Dynamics. Part 2 Theory, Advances in Chemical Physics LXXXII (M. Baer and C. Y. Ng, eds.), Wiley, New York, 1992, p. 423. [Pg.528]

Here, Mo -O denotes one of the two molybdenyl bonds of a tetrahedrally coordinated Mo ion on the silica surface. ( Mo -0 ) stands for a short-lived charge-transfer excited state which is formed upon absorption of UV-light quantum (hv). The excited state was earlier detected in photoluminescence experiments. I is the light intensity, and is the rate constant for deactivation of the excited state. Reaction (3) is the interaction of CO with the excited state to yield Mo and CO2. Reaction (4) is quenching of the excited state ( Mo -0 ) by NO molecules without formation of reaction products. Reaction (4) is of importance for the kinetic consideration. [Pg.425]

The general scheme for a senticonductor electrode takes into account a two-step charge-transfer process [17]. One step corresponds to the transfer of electrons and ions through the Helmholtz layer. Let Zh be the corresponding impedance that is in parallel to Ch, the capacity of the Helmholtz layer and let Z be the impedance of this parallel combination. The other step exists due to the localization of charges in surface states or intermediates. Here the corresponding impedance, Zsc, is in... [Pg.173]

Chemisorption occurs when the attractive potential well is large so that upon adsorption a strong chemical bond to a surface is fonued. Chemisorption involves changes to both the molecule and surface electronic states. For example, when oxygen adsorbs onto a metal surface, a partially ionic bond is created as charge transfers from the substrate to the oxygen atom. Other chemisorbed species interact in a more covalent maimer by sharing electrons, but this still involves perturbations to the electronic system. [Pg.294]


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See also in sourсe #XX -- [ Pg.15 ]




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Charge transfer state

Charged surfaces

Surface charge

Surface charges surfaces

Surface charging

Surface states

Surface states charge

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