2022
DOI: 10.1021/acs.jctc.2c00321
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Toward Efficient Direct Dynamics Studies of Chemical Reactions: A Novel Matrix Completion Algorithm

Abstract: This paper describes the development and testing of a polynomial variety-based matrix completion (PVMC) algorithm. Our goal is to reduce computational effort associated with reaction rate coefficient calculations using variational transition state theory with multidimensional tunneling (VTST-MT). The algorithm recovers eigenvalues of quantum mechanical Hessians constituting the minimum energy path (MEP) of a reaction using only a small sample of the information, by leveraging underlying properties of these eig… Show more

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Cited by 3 publications
(4 citation statements)
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“…This is because the computational cost and therefore the success of CS (or low-rank MC), depends on the sparsity (or rank) of that particular problem. For instance, PVMC can be a few times cheaper than Hessian calculations across the entire MEP . However, the true cost depends on the complexity (rank) of the reaction which can only be approximately determined.…”
Section: Discussionmentioning
confidence: 99%
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“…This is because the computational cost and therefore the success of CS (or low-rank MC), depends on the sparsity (or rank) of that particular problem. For instance, PVMC can be a few times cheaper than Hessian calculations across the entire MEP . However, the true cost depends on the complexity (rank) of the reaction which can only be approximately determined.…”
Section: Discussionmentioning
confidence: 99%
“…In our group, we are addressing (1) by developing matrix completion (MC) algorithms that leverage polynomial and low-rank structures of higher derivatives, specifically eigenvalues of Hessians that constitute the MEP. The approach is grounded in the potential energy term of the reaction path Hamiltonian (RPH) in which translations, rotations, and the reaction coordinate are projected out. The potential energy is described in terms of normal mode displacements { q i }: , V ( s , q ) = V 0 ( s ) + 1 2 i = 1 F 1 ω i 2 q i 2 where F = 3 N at – 6, V 0 ( s ) is the energy at a point on the MEP described by arc length s (=0 at transition state, ± ∞ at reactant/product), and { ω i 2 } are squares of vibrational frequencies obtained from Hessian eigenvalues.…”
Section: Compressed Sensing and Matrix Completionmentioning
confidence: 99%
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