2016
DOI: 10.1021/acs.jctc.6b00388
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Toward a General Yet Effective Computational Approach for Diffusive Problems: Variable Diffusion Tensor and DVR Solution of the Smoluchowski Equation along a General One-Dimensional Coordinate

Abstract: A generalization to arbitrary large amplitude motions of a recent approach to the evaluation of diffusion tensors [ J. Comput. Chem. , 2009 , 30 , 2 - 13 ] is presented and implemented in a widely available package for electronic structure computations. A fully black-box tool is obtained, which, starting from the generation of geometric structures along different kinds of paths, proceeds toward the evaluation of an effective diffusion tensor and to the solution of one-dimensional Smoluchowski equations by a ro… Show more

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Cited by 5 publications
(14 citation statements)
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References 62 publications
(132 reference statements)
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“…Some of the authors of this article introduced the former DiTe software package as a general tool for the computation of the generalized friction tensor of flexible molecules, with flexibility given in terms of dihedral angles only. Finally, Piserchia et al developed a module for the Gaussian quantum chemistry software package that extends the modeling introduced by DiTe to internal flexibility in terms of delocalized internal coordinates.…”
Section: Introductionmentioning
confidence: 99%
“…Some of the authors of this article introduced the former DiTe software package as a general tool for the computation of the generalized friction tensor of flexible molecules, with flexibility given in terms of dihedral angles only. Finally, Piserchia et al developed a module for the Gaussian quantum chemistry software package that extends the modeling introduced by DiTe to internal flexibility in terms of delocalized internal coordinates.…”
Section: Introductionmentioning
confidence: 99%
“…For these two different views a set of Cartesian velocities and forces for the unconstrained system and a set of external velocities and forces for the constrained system are considered. A laboratory frame (LF) and a molecular frame (MF) (fixed in the Eckart orientation on the molecular center of mass) are chosen and after some classical mechanics passages17,24 we can express the Cartesian velocities v i of the i -th atom for the unconstrained system as boldvi=υ+boldEtr(Ω)(ω×boldci+boldcixx˙) where υ , ω , ẋ are the set of external velocities, respectively the translational velocity, the angular velocity and the generalized coordinate moment. E ( Ω ) is the Euler matrix dependent on the set of Euler angles Ω that brings the LF into the MF and c i are the Cartesian coordinates expressed in the MF of the i -th atom.…”
Section: Theorymentioning
confidence: 99%
“…All the technical details about the diffusion tensor model here omitted for sake of brevity can be found in our previous work, ref. 17, to which the interested reader is addressed.…”
Section: Theorymentioning
confidence: 99%
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