2021
DOI: 10.1007/978-981-33-6639-8_6
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Efficient Sampling of High-Dimensional Free Energy Landscapes: A Review of Parallel Bias Metadynamics

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Cited by 6 publications
(6 citation statements)
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“…In contrast to typical MetaD which uses a high-dimensional bias potential to reconstruct the free energy landscape, in the PBMetaD sampling scheme, multiple 1D bias potentials are constructed on the fly to reconstruct the free energy surface (FES) of a highly dimensional CV space. This approach has previously been applied to converge the FES for many high-dimensional systems. Mastery of these energy landscapes provides insight into the sidechain interactions that give rise to unique secondary structures in peptoids and the development of predictive models for the rational design of engineered peptoid structures.…”
Section: Introductionmentioning
confidence: 99%
“…In contrast to typical MetaD which uses a high-dimensional bias potential to reconstruct the free energy landscape, in the PBMetaD sampling scheme, multiple 1D bias potentials are constructed on the fly to reconstruct the free energy surface (FES) of a highly dimensional CV space. This approach has previously been applied to converge the FES for many high-dimensional systems. Mastery of these energy landscapes provides insight into the sidechain interactions that give rise to unique secondary structures in peptoids and the development of predictive models for the rational design of engineered peptoid structures.…”
Section: Introductionmentioning
confidence: 99%
“…In the PBMetaD sampling scheme, multiple 1D bias potentials are deposited on the fly and later reconstructed to fully sample and characterize a highly dimensional CV space. This approach has previously been shown to converge exactly and been applied to a number of other high-dimensional systems. In the parallel bias metadynamics scheme, the following CVs were biased using 1D well-tempered metadynamics potentials: ring coordination number for each aromatic pair (sigma = 0.5), overall coordination number (sigma = 0.5), radius of gyration (sigma = 0.5 nm), backbone ω dihedrals (sigma = 0.35 rad), backbone ϕ dihedrals (sigma = 0.35 rad), backbone ψ dihedrals (sigma = 0.35 rad), and sidechain χ 1 dihedrals (sigma = 0.35 rad). A Gaussian potential with an initial hill height of 2.5 kJ/mol, a bias factor of 50, and a hill deposition pace of 1 hill/1 ps (500 steps) was used.…”
Section: Methodsmentioning
confidence: 99%
“…This method was found to be very efficient for revealing the free energy estimates associated with various biological and chemical systems that have high energy barriers. 49,63–66 By contrast, umbrella sampling provides control over a given CV to model the conformational transitions aided by a series of independent windows. 48,67,68…”
Section: Methodsmentioning
confidence: 99%
“…This method was found to be very efficient for revealing the free energy estimates associated with various biological and chemical systems that have high energy barriers. 49,[63][64][65][66] By contrast, umbrella sampling provides control over a given CV to model the conformational transitions aided by a series of independent windows. 48,67,68 The method of combining umbrella sampling and metadynamics biases for the sampling of high-dimensional free energy surfaces was proposed by Filizola and co-workers 69 and by Nair and co-workers.…”
Section: Equilibration and Simulationmentioning
confidence: 99%