1999
DOI: 10.1002/9780470141656.ch3
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Electron Transfer—from Isolated Molecules to Biomolecules

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Cited by 474 publications
(359 citation statements)
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References 773 publications
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“…The latter is dependent on the dielectric and polarisable properties of the medium, [24][25][26][27][28][29] the former is the energy associated with the structural changes of the reactants on progression to product geometry (and vice versa). [24][25][26]30] The contribution to λ from λ i can be significant and dominates inner sphere charge transfer processes (those CT processes where there are no solvent molecules intervening to prevent molecular contact between reactants). [23] In general, λ i increases with increasing localisation of charge whether dealing with monomeric or oligomeric materials.…”
Section: Introductionmentioning
confidence: 99%
See 1 more Smart Citation
“…The latter is dependent on the dielectric and polarisable properties of the medium, [24][25][26][27][28][29] the former is the energy associated with the structural changes of the reactants on progression to product geometry (and vice versa). [24][25][26]30] The contribution to λ from λ i can be significant and dominates inner sphere charge transfer processes (those CT processes where there are no solvent molecules intervening to prevent molecular contact between reactants). [23] In general, λ i increases with increasing localisation of charge whether dealing with monomeric or oligomeric materials.…”
Section: Introductionmentioning
confidence: 99%
“…Self-exchange charge transfer reactions may be considered [23] to be the primary mediators of charge flow in organic conducting polymers and amorphous thin films. At room temperature in such environments these reactions are usually considered to involve a series of thermally activated electron and/or hole hops between adjacent charged radical ions and neutral parent species; Rate constants, k CT for both hole and electron transfer self-exchange processes can be expressed using the semi-classical form of the Marcus equation (Equation 1): [24][25][26] √ [ ] where k CT is the rate constant for electron transfer, k B and T are the Boltzmann constants and temperature respectively, λ is the reorganisation energy and V is the electronic coupling factor, sometimes referred to as the charge transfer integral, t. It can be seen that for an iso-energetic charge transfer process, k CT depends only on V and λ. In turn, λ is divided into contributions from two components; inner and outer sphere reorganisation energies, λ i and λ o respectively.…”
Section: Introductionmentioning
confidence: 99%
“…T he intrinsic electron transfer (ET) mechanisms of even small and otherwise well-characterized proteins such as cytochrome c or azurin (Az) are difficult to identify conclusively because of the proteins' complexity, i.e., inhomogeneous structural and dynamic properties (1)(2)(3)(4)(5)(6)(7)(8)(9)(10)(11)(12)(13)(14). The use of bioelectrochemical tunneling junctions, such as self-assembled monolayer (SAM) films of variable composition and thickness on metal electrodes, with redox proteins immobilized at the solution interface (or freely diffusing to the SAM terminal groups) have been shown to provide an assembly with well-defined and variable control parameters.…”
mentioning
confidence: 99%
“…22 The former assumes that only the first two cumulants of q are significant for time-independent (stationary) lineshapes measured in the limit t → ∞. The corresponding absorption and emission lineshapes are given by Gaussian functions, 36 with their maxima separated by the Stokes shift ∆Ω =Ω g −Ω e ,…”
Section: Time-resolved Lineshapesmentioning
confidence: 99%