2019
DOI: 10.1063/1.5094046
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Efficient geometric integrators for nonadiabatic quantum dynamics. II. The diabatic representation

Abstract: Exact nonadiabatic quantum evolution preserves many geometric properties of the molecular Hilbert space. In a companion paper [S. Choi and J. Vaníček, 2019], arXiv:1903.04946v3 [physics.chem-ph]

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Cited by 28 publications
(30 citation statements)
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“…10,11,57 For additional details about the properties and numerical implementation of the higher-order split-operator algorithms, we refer the reader to Ref. 12.…”
Section: A Split-operator Algorithm and Dynamic Fourier Methodsmentioning
confidence: 99%
See 1 more Smart Citation
“…10,11,57 For additional details about the properties and numerical implementation of the higher-order split-operator algorithms, we refer the reader to Ref. 12.…”
Section: A Split-operator Algorithm and Dynamic Fourier Methodsmentioning
confidence: 99%
“…In addition, because of its symmetry, this algorithm can be composed by various symmetric composition schemes to obtain higher-order integrators. 11,12,[48][49][50][51] As well as having favorable geometric properties, the proposed algorithm is also very simple to implement because its implementation does not depend on the form of the potential energy arXiv:1909.06412v2 [quant-ph] 8 Nov 2019 function and because the grid adaptation requires no adjustable parameters.…”
Section: Introductionmentioning
confidence: 99%
“…Therefore, they can be further composed using symmetric composition methods 4,34,[45][46][47][48][50][51][52][53] in order to obtain integrators of arbitrary even orders of convergence. To this end, starting from an integrator Ûp of even order p, an integrator Ûp+2 of order p + 2 is generated using the symmetric composition…”
Section: B Recovery Of Geometric Properties and Increasing Accuracy B...mentioning
confidence: 99%
“…As in the split-operator algorithm 58,82,83 for the TDSE or in the Verlet algorithm 59 for Hamilton's equations of motion, we can obtain a symmetric potential-kinetic-potential (VTV) algorithm of the second order in the time step ∆t by using the Strang splitting 56 and performing, in sequence, potential propagation for time ∆t/2, kinetic propagation for ∆t, and potential propagation for ∆t/2. The second-order kinetic-potential-kinetic (TVT) algorithm is obtained similarly, by exchanging the potential and kinetic propagations.…”
Section: Geometric Integratorsmentioning
confidence: 99%