2019
DOI: 10.1021/acs.jpclett.8b03061
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Improved Ehrenfest Approach to Model Correlated Electron–Nuclear Dynamics

Abstract: Mixed quantum-classical mechanics descriptions are critical to modeling coupled electron-nuclear dynamics, i.e. non-adiabatic molecular dynamics, relevant to photochemical and photophysical processes. We argue that, for polyatomic molecules, such mixed dynamics can not be efficiently described in terms of a matrix gauge potential and develop the concept of a "length gauge" effective Hamiltonian, which helps clarifying certain aspects for the popular non-adiabatic computational approaches. In particular, within… Show more

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Cited by 13 publications
(18 citation statements)
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“…Thus, when substituting eq into the Schrödinger equation, eq , one should assume that ψ a are explicit functions of t , ψ a = ψ a ( r , R t ). Following such assumption, the substitution of eq into eq gives , with Note that in the expression for V ab the Hamiltonian, Ĥ el , contains R as an operator, while R t is a variable. Expansion of Ĥ el ( R ) in the vicinity of R t leads to an effective Hamiltonian, with In eq , parameters E a , f a , and κ̂ a are the a th expectation values of the electronic Hamiltonian, Ĥ el ( R t ), and its first and second derivatives, respectively.…”
Section: Theoretical Developments and Non-adiabatic Excited-state Mol...mentioning
confidence: 99%
“…Thus, when substituting eq into the Schrödinger equation, eq , one should assume that ψ a are explicit functions of t , ψ a = ψ a ( r , R t ). Following such assumption, the substitution of eq into eq gives , with Note that in the expression for V ab the Hamiltonian, Ĥ el , contains R as an operator, while R t is a variable. Expansion of Ĥ el ( R ) in the vicinity of R t leads to an effective Hamiltonian, with In eq , parameters E a , f a , and κ̂ a are the a th expectation values of the electronic Hamiltonian, Ĥ el ( R t ), and its first and second derivatives, respectively.…”
Section: Theoretical Developments and Non-adiabatic Excited-state Mol...mentioning
confidence: 99%
“…The diversity of strategies tested with some or all of Tully models is astonishing. It includes, among others, full multiple spawning, 15 semiclassical initial value representation, 23 symmetrical quasi-classical windowing combined with Meyer-Miller mapping Hamiltonian, 24 surface hopping Herman-Kluk semiclassical initial value representation method, 25 semiclassical Monte-Carlo, 26 dephasing representation of quantum fidelity, 27 counter-propagating wave methods trajectories, 28 Ehrenfest-Plus, 29 coupled-trajectory mixed quantum/classical dynamics, 30,31 quantum trajectory mean-field approach, 32 iterative linearized approach to nonadiabatic dynamics, 33 mean-field dynamics with stochastic decoherence, 34 nonadiabatic Bohmian dynamics, 35,36 mean-field molecular dynamics with surface hopping, 37 non-Hermitian surface hopping, 38 multi-state trajectory approach to nonadiabatic dynamics, 39…”
Section: Introductionmentioning
confidence: 99%
“…The enhancement of radiation and PP by highenergy e ± and photons in strong and sub-strong crystalline fields was first experimentally investigated in the 1980s. The studies on PP were firstly focused on lighter elements such as silicon and germanium [28], and only at a later stage on high-Z crystalline metals such as tungsten and iridium [29,30,31]. These studies were driven by the need to test the feasibility of an intense positron source [32] and to develop a compact photon converter, i.e., a device to separate the photon and neutral hadron beam components with minimal absorption or scattering of the latter [29,30], for the NA48 experiment at CERN; eventually, an iridium crystal with a thickness of 0.98 X 0 was employed [33].…”
Section: Introductionmentioning
confidence: 99%