2017
DOI: 10.1063/1.5006465
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Accelerated path-integral simulations using ring-polymer interpolation

Abstract: Path-integral (PI) molecular simulations can be used to calculate exact quantum statistical mechanical properties for complex systems containing many interacting atoms and molecules. The limiting computational factor in a PI simulation is typically the evaluation of the potential energy surface (PES) and forces at each ring-polymer "bead"; for an n-bead ring-polymer, a PI simulation is typically n times greater than the corresponding classical simulation. To address the increased computational effort of PI sim… Show more

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Cited by 13 publications
(7 citation statements)
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“…1 Though NQEs appear to be minimal for the calculated intermolecular properties in some water simulations, 2-3 they were found to be non-negligible in other cases [4][5] as demonstrated by the differences in thermodynamic properties between light and heavy water. 1 In principle, Feynman's imaginary-time path-integral formalism 6 enables the modeling of NQEs in liquid water to numerical accuracy, but the associated high computational cost has hindered widespread application of path-integral molecular dynamics (PIMD) simulations until recent developments of more efficient approximations, 7 such as the ring-polymer contraction (RPC), 8 the ring-polymer interpolation, 9 and the combined path-integral and generalized Langevin equation (PI+GLE) approach. 10 The computational cost of a PIMD simulation of liquid water significantly increases when the underlying Born-Oppenheimer potential energy surface is calculated "on the fly" as in ab initio molecular dynamics (AIMD) simulations 11 where Kohn-Sham density functional theory 12 (KS-DFT) is generally used to solve the (electronic) Schrödinger equation at each step of the dynamical trajectory.…”
Section: Introductionmentioning
confidence: 99%
“…1 Though NQEs appear to be minimal for the calculated intermolecular properties in some water simulations, 2-3 they were found to be non-negligible in other cases [4][5] as demonstrated by the differences in thermodynamic properties between light and heavy water. 1 In principle, Feynman's imaginary-time path-integral formalism 6 enables the modeling of NQEs in liquid water to numerical accuracy, but the associated high computational cost has hindered widespread application of path-integral molecular dynamics (PIMD) simulations until recent developments of more efficient approximations, 7 such as the ring-polymer contraction (RPC), 8 the ring-polymer interpolation, 9 and the combined path-integral and generalized Langevin equation (PI+GLE) approach. 10 The computational cost of a PIMD simulation of liquid water significantly increases when the underlying Born-Oppenheimer potential energy surface is calculated "on the fly" as in ab initio molecular dynamics (AIMD) simulations 11 where Kohn-Sham density functional theory 12 (KS-DFT) is generally used to solve the (electronic) Schrödinger equation at each step of the dynamical trajectory.…”
Section: Introductionmentioning
confidence: 99%
“…1 Though NQEs appear to be minimal for the calculated intermolecular properties in some water simulations, 2, 3 they were found to be non-negligible in other cases 4,5 as demonstrated by the differences in thermodynamic properties between light and heavy water. 1 In principle, Feynman's imaginary-time path-integral formalism 6 enables the modeling of NQEs in liquid water to numerical accuracy, but the associated high computational cost has hindered widespread application of path-integral molecular dynamics (PIMD) simulations until recent developments of more efficient approximations, 7 such as the ring-polymer contraction (RPC), 8 the ring-polymer interpolation, 9 and the combined path-integral and generalized Langevin equation (PI+GLE) approach. 10 The computational cost of a PIMD simulation of liquid water significantly increases when the underlying Born-Oppenheimer potential energy surface is calculated "on the fly" as in ab initio molecular dynamics (AIMD) simulations 11 where Kohn-Sham density functional theory 12 (KS-DFT) is generally used to solve the (electronic) Schrödinger equation at each step of the dynamical trajectory.…”
Section: Introductionmentioning
confidence: 99%
“…Quantum mechanical simulations with atomistic resolution are currently reaching length and time scales that had been almost unimaginable only a few decades ago. The reasons for this impressive progress can be attributed to a number of conspiring factors including the increase of the availability of high performance computers, improved algorithms in many community software packages [1][2][3] , and the sympatico relationship of machine learning with quantum mechanical methods [4][5][6][7] .…”
Section: Introductionmentioning
confidence: 99%