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  • In the theoretical part of my contribution I will introduce the Always Stable Predictor-Corrector (ASPC) method. It is suitable for integrating the equations of motion with a right-hand side containing an implicit equation of a self-consistent field (SCF) type, like calculation of induced dipoles. The method combines two principles: stability (errors decay while propagating to next steps) and time reversibility of a sufficiently high order (energy conservation). The method is locally of second order. It contains one mixing (damping) parameter which can be chosen so that the method is always stable for a converging SCF or optimized to convergence properties of given system. Higher-order but only partially stable schemes are also discussed. The ASPC method can be written both in a history form and Gear notation. The ASPC method is tested using polarizable water and compared with the full iteration method with a predictor an the extended Lagrangian (Car-Parrinello-like) method. Accuracy and efficiency
  • In the theoretical part of my contribution I will introduce the Always Stable Predictor-Corrector (ASPC) method. It is suitable for integrating the equations of motion with a right-hand side containing an implicit equation of a self-consistent field (SCF) type, like calculation of induced dipoles. The method combines two principles: stability (errors decay while propagating to next steps) and time reversibility of a sufficiently high order (energy conservation). The method is locally of second order. It contains one mixing (damping) parameter which can be chosen so that the method is always stable for a converging SCF or optimized to convergence properties of given system. Higher-order but only partially stable schemes are also discussed. The ASPC method can be written both in a history form and Gear notation. The ASPC method is tested using polarizable water and compared with the full iteration method with a predictor an the extended Lagrangian (Car-Parrinello-like) method. Accuracy and efficiency (en)
Title
  • Molecular dynamics of polarizable models
  • Molecular dynamics of polarizable models (en)
skos:prefLabel
  • Molecular dynamics of polarizable models
  • Molecular dynamics of polarizable models (en)
skos:notation
  • RIV/60461373:22340/10:00023317!RIV11-GA0-22340___
http://linked.open...avai/riv/aktivita
http://linked.open...avai/riv/aktivity
  • P(GA203/07/1006), P(GAP208/10/1724), P(LC512), S
http://linked.open...vai/riv/dodaniDat
http://linked.open...aciTvurceVysledku
http://linked.open.../riv/druhVysledku
http://linked.open...iv/duvernostUdaju
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http://linked.open...dnocenehoVysledku
  • 272378
http://linked.open...ai/riv/idVysledku
  • RIV/60461373:22340/10:00023317
http://linked.open...riv/jazykVysledku
http://linked.open.../riv/klicovaSlova
  • molecular dynamics; polarizability; ASPC (en)
http://linked.open.../riv/klicoveSlovo
http://linked.open...i/riv/kodPristupu
http://linked.open...ontrolniKodProRIV
  • [2FC1EF852DB1]
http://linked.open...i/riv/mistoVydani
  • Lausanne
http://linked.open...telVyzkumneZpravy
  • Centre Européen de Calcul Atomique et Moléculaire
http://linked.open...in/vavai/riv/obor
http://linked.open...ichTvurcuVysledku
http://linked.open...cetTvurcuVysledku
http://linked.open...vavai/riv/projekt
http://linked.open...UplatneniVysledku
http://linked.open...iv/tvurceVysledku
  • Kolafa, Jiří
http://localhost/t...ganizacniJednotka
  • 22340
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