2017
DOI: 10.1002/jcc.24775
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FFLUX: Transferability of polarizable machine‐learned electrostatics in peptide chains

Abstract: The fully polarizable, multipolar, and atomistic force field protein FFLUX is being built from machine learning (i.e., kriging) models, each of which predicts an atomic property. Each atom of a given protein geometry needs to be assigned such a kriging model. Such a knowledgeable atom needs to be informed about a sufficiently large environment around it. The resulting complexity can be tackled by collecting the 20 natural amino acids into a few groups. Using substituted deca-alanines, we present the proof-of-c… Show more

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Cited by 20 publications
(23 citation statements)
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References 41 publications
(57 reference statements)
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“…DFT-based first-principles calculations of ELNES and partial density of states (PDOS) are performed using the Cambridge Serial Total Energy Package (CASTEP) within the generalized gradient approximation (GGA) using the Perdew-Burke-Enzerhof (PBE) functional (Perdew et al, 1996). The Broyden-Fletcher-Goldfrab-Shanno (BFGS) geometry optimization scheme has been used (Broyden, 1970;Fletcher, 1970;Goldfarb, 1970;Shanno, 1970). All atoms were fully relaxed until the magnitude of the force on each atom converged to less than 0.01 eV Å À1 and the energy change per atom converged to less than 5 Â 10 À7 eV atom À1 , yielding optimized structures using the virtual crystal approximation (Bellaiche & Vanderbilt, 2000;Sen & Ghosh, 2016).…”
Section: Theory and Computational Methodologymentioning
confidence: 99%
“…DFT-based first-principles calculations of ELNES and partial density of states (PDOS) are performed using the Cambridge Serial Total Energy Package (CASTEP) within the generalized gradient approximation (GGA) using the Perdew-Burke-Enzerhof (PBE) functional (Perdew et al, 1996). The Broyden-Fletcher-Goldfrab-Shanno (BFGS) geometry optimization scheme has been used (Broyden, 1970;Fletcher, 1970;Goldfarb, 1970;Shanno, 1970). All atoms were fully relaxed until the magnitude of the force on each atom converged to less than 0.01 eV Å À1 and the energy change per atom converged to less than 5 Â 10 À7 eV atom À1 , yielding optimized structures using the virtual crystal approximation (Bellaiche & Vanderbilt, 2000;Sen & Ghosh, 2016).…”
Section: Theory and Computational Methodologymentioning
confidence: 99%
“…The interaction energy, V AB corr , of each atom with itself (A = B) or with one of the other atoms (A ≠ B) is obtained from the 2PDM via a 6D quadrature integration. The 3D ESP [51] approach was more recently developed with the intent of ultimate implementation in our polarizable multipolar [52] topological force field FFLUX [53][54][55][56][57], since 3D ESP is faster and more accurate when compared to the 6D approach. The master equation for the 3D ESP integration is given just below, where any derivation details are not repeated here but can be found in the selfcontained account of ref.…”
Section: Iqa Dynamic Electron Correlation Energymentioning
confidence: 99%
“…We use 16 × 16 × 1, 16 × 16 × 1, and 8 × 16 × 1 k-points for the 1H, 1T and 1T MoS 2 , respectively. To obtain optimized atomic configurations of MoS 2 monolayers, the atomic positions and cell vectors are fully relaxed using the Broyden-Fretcher-Goldfarb-Shanno minimization method [22][23][24][25] until all the Hellmann-Feynman forces and all components of the stress are less than 5 × 10 −4 Ry/a.u. and 5 × 10 −2 GPa, respectively.…”
Section: Calculation Detailsmentioning
confidence: 99%