2000
DOI: 10.1063/1.481609
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Continuous surface switching: An improved time-dependent self-consistent-field method for nonadiabatic dynamics

Abstract: We present a new semiclassical method for electronically nonadiabatic collisions. The method is a variant of the time-dependent self-consistent-field method and is called continuous surface switching. The algorithm involves a self-consistent potential trajectory surface switching approach that is designed to combine the advantages of the trajectory surface hopping approach and the Ehrenfest classical path self-consistent potential approach without their relative disadvantages. Viewed from the self-consistent p… Show more

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Cited by 119 publications
(116 citation statements)
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“…25,27,[32][33][34]36,[41][42][43][44]46,53 Because it has been impractical to study dynamics for systems with very small semiclassical transition probabilities, these tests have been carried out for systems with nonadiabatic probabilities of 3ϫ10 Ϫ4 and larger. The army ants algorithm allows us to extend these tests down to much lower probabilities; for example, in the present paper we present well-converged calculations for a system with a nonadiabatic transition probability of 1ϫ10…”
Section: Introductionmentioning
confidence: 99%
“…25,27,[32][33][34]36,[41][42][43][44]46,53 Because it has been impractical to study dynamics for systems with very small semiclassical transition probabilities, these tests have been carried out for systems with nonadiabatic probabilities of 3ϫ10 Ϫ4 and larger. The army ants algorithm allows us to extend these tests down to much lower probabilities; for example, in the present paper we present well-converged calculations for a system with a nonadiabatic transition probability of 1ϫ10…”
Section: Introductionmentioning
confidence: 99%
“…68 OWVP calculations have been performed more recently on a variety of model systems, including three qualitatively different types of chemical systems: (1) systems with conical intersections, [69][70][71][72][73] (2) systems with diabatic surfaces that cross and adiabatic surfaces that do not intersect, 74 and (3) systems with wide regions of weak coupling where neither the diabatic nor the adiabatic surfaces cross. 75,76 This set of calculations includes reactive 69,72,[74][75][76] and nonreactive 71,72 scattering collisions as well as unimolecular excited-state decay processes. 70,73 The availability of accurate quantum mechanical results for realistic full-dimensional non-BO systems allows for the systematic study of the accuracy of more approximate methods, and we have identified a subset of the calculations discussed above to serve as benchmark test cases.…”
Section: Quantum Mechanical Dynamicsmentioning
confidence: 99%
“…(5)) is referred to as a potential energy matrix or PEM. We include three LandauZener-Teller-type [77][78][79] PEMs (collectively referred to as the MXH family 74 of PEMs), which feature narrowly avoided crossings where the diabatic surfaces cross but the adiabatic surfaces do not.…”
Section: Quantum Mechanical Dynamicsmentioning
confidence: 99%
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“…This is actually a tunneling process that is classically forbidden. 6,13 Many hybrid methods have been proposed that try to combine the advantages of surface hopping and Ehrenfest mean-field like approaches, for example, the use of a smooth switching between the two types of forces in different regions, 14 Ehrenfest dynamics guided surface hopping 15 or the surface hopping dynamics with Ehrenfest excited state potential 16 approaches are two recent versions of such ideas.…”
Section: Introductionmentioning
confidence: 99%