2002
DOI: 10.1021/jp0142886
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Multistate Effects in Calculations of the Electronic Coupling Element for Electron Transfer Using the Generalized Mulliken−Hush Method

Abstract: A simple diagnostic is developed for the purpose of determining when a third state must be considered to calculate the electronic coupling element for a given pair of diabatic states within the context of the generalized Mulliken-Hush approach (Chem. Phys. Lett. 1996, 275, 15-19). The diagnostic is formulated on the basis of Löwdin partitioning theory. In addition, an effective 2-state GMH expression is derived for the coupling as it is modified by the presence of the third state. Results are presented for (i)… Show more

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Cited by 98 publications
(106 citation statements)
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“…The donoracceptor couplings calculated using the two-and three-state schemes are 1.72 and 2.46 meV, respectively. If donor and acceptor are almost in resonance ͑F = 6.725ϫ 10 −5 a.u.͒, the difference 2 − 1 = 0.29 D is remarkably smaller than 13 = 0.71 D. However, the two-and three-state couplings are similar ͑1.63 and 2.37 meV͒ to the estimates found at F =0. Furthermore, according to our experience, in nonsymmetric systems the difference 2 − 1 is often essentially larger than transition moments; however, the performance of the twostate model strongly depends on the system being considered.…”
Section: Effects Of External Parameters On Adiabatic and Diabatic Promentioning
confidence: 63%
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“…The donoracceptor couplings calculated using the two-and three-state schemes are 1.72 and 2.46 meV, respectively. If donor and acceptor are almost in resonance ͑F = 6.725ϫ 10 −5 a.u.͒, the difference 2 − 1 = 0.29 D is remarkably smaller than 13 = 0.71 D. However, the two-and three-state couplings are similar ͑1.63 and 2.37 meV͒ to the estimates found at F =0. Furthermore, according to our experience, in nonsymmetric systems the difference 2 − 1 is often essentially larger than transition moments; however, the performance of the twostate model strongly depends on the system being considered.…”
Section: Effects Of External Parameters On Adiabatic and Diabatic Promentioning
confidence: 63%
“…Electron transition 1 → 2 results in a considerable change of the adiabatic dipole moment 2 − 1 Ϸ 31.8 D. Because the state 3 is mainly localized on the bridge, 3 − 1 = 2 − 3 =1/2͑ 2 − 1 ͒. The transition moment 12 of ϳ2.7 D is essentially larger than 13 and 23 . The d-a electronic coupling V da is by order of magnitude smaller than the matrix elements V db and V ab associated with the bridge state.…”
Section: Effects Of External Parameters On Adiabatic and Diabatic Promentioning
confidence: 97%
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“…Diabatization approximations are particularly suited for evaluating excitonic couplings between several excited states. [26][27][28][29] Recently, some of us have developed a diabatization scheme to compute excitonic couplings between molecular crystal pairs beyond the two-level approximation. 30 The great advantage of diabatization schemes is that they can deal with the short-range (exchange and overlap) and long-range (Coulombic) contributions of the excitonic couplings on equal footing.…”
Section: Introductionmentioning
confidence: 99%
“…24,25 For , which may involve exciplex formation) 27 )susing the appropriate 2-st models in a pairwise fashion. However, if the states interact strongly with each other, a 3-state treatment may be required, especially in the case of radiative CR, which may involve significant intensity borrowing or other types of vibronic coupling.…”
Section: Introductionmentioning
confidence: 99%