Implementation of extended Lagrangian dynamics in GROMACS for polarizable simulations using the classical Drude oscillator model
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[1] Alexander D. MacKerell,et al. CHARMM fluctuating charge force field for proteins: II Protein/solvent properties from molecular dynamics simulations using a nonadditive electrostatic model , 2004, J. Comput. Chem..
[2] Richard A. Friesner,et al. Constructing ab initio force fields for molecular dynamics simulations , 1998 .
[3] Pengyu Y. Ren,et al. Consistent treatment of inter‐ and intramolecular polarization in molecular mechanics calculations , 2002, J. Comput. Chem..
[4] Alexander D. MacKerell,et al. Optimization of the additive CHARMM all-atom protein force field targeting improved sampling of the backbone φ, ψ and side-chain χ(1) and χ(2) dihedral angles. , 2012, Journal of chemical theory and computation.
[5] Michael F. Crowley,et al. New faster CHARMM molecular dynamics engine , 2013, J. Comput. Chem..
[6] Benoît Roux,et al. A polarizable force field of dipalmitoylphosphatidylcholine based on the classical Drude model for molecular dynamics simulations of lipids. , 2013, The journal of physical chemistry. B.
[7] T. Darden,et al. Particle mesh Ewald: An N⋅log(N) method for Ewald sums in large systems , 1993 .
[8] Harry A. Stern,et al. Development of a polarizable force field for proteins via ab initio quantum chemistry: First generation model and gas phase tests , 2002, J. Comput. Chem..
[9] Gerhard Hummer,et al. System-Size Dependence of Diffusion Coefficients and Viscosities from Molecular Dynamics Simulations with Periodic Boundary Conditions , 2004 .
[10] Alexander D. MacKerell,et al. All‐atom polarizable force field for DNA based on the classical drude oscillator model , 2014, J. Comput. Chem..
[11] Laxmikant V. Kalé,et al. Scalable molecular dynamics with NAMD , 2005, J. Comput. Chem..
[12] Gerrit Groenhof,et al. GROMACS: Fast, flexible, and free , 2005, J. Comput. Chem..
[13] Benoît Roux,et al. Modeling induced polarization with classical Drude oscillators: Theory and molecular dynamics simulation algorithm , 2003 .
[14] L. Verlet. Computer "Experiments" on Classical Fluids. I. Thermodynamical Properties of Lennard-Jones Molecules , 1967 .
[15] Alexander D. MacKerell,et al. Induced Polarization Influences the Fundamental Forces in DNA Base Flipping , 2014, The journal of physical chemistry letters.
[16] W. C. Swope,et al. A computer simulation method for the calculation of equilibrium constants for the formation of physi , 1981 .
[17] Taehoon Kim,et al. CHARMM‐GUI: A web‐based graphical user interface for CHARMM , 2008, J. Comput. Chem..
[18] David van der Spoel,et al. Molecular Dynamics Simulations of Water with Novel Shell-Model Potentials , 2001 .
[19] C. Bugg,et al. Structure of ubiquitin refined at 1.8 A resolution. , 1987, Journal of molecular biology.
[20] Peter M. Kasson,et al. GROMACS 4.5: a high-throughput and highly parallel open source molecular simulation toolkit , 2013, Bioinform..
[21] Klaus Schulten,et al. High-performance scalable molecular dynamics simulations of a polarizable force field based on classical Drude oscillators in NAMD. , 2011, The journal of physical chemistry letters.
[22] Anastassia N Alexandrova,et al. Polarization Effects for Hydrogen-Bonded Complexes of Substituted Phenols with Water and Chloride Ion. , 2007, Journal of chemical theory and computation.
[23] Anna-Pitschna E. Kunz,et al. Development of a nonlinear classical polarization model for liquid water and aqueous solutions: COS/D. , 2009, The journal of physical chemistry. A.
[24] B. Thole. Molecular polarizabilities calculated with a modified dipole interaction , 1981 .
[25] Alexander D. MacKerell,et al. Force Field for Peptides and Proteins based on the Classical Drude Oscillator. , 2013, Journal of chemical theory and computation.
[26] Pengyu Y. Ren,et al. The Polarizable Atomic Multipole-based AMOEBA Force Field for Proteins. , 2013, Journal of chemical theory and computation.
[27] Charles L. Brooks,et al. CHARMM fluctuating charge force field for proteins: I parameterization and application to bulk organic liquid simulations , 2004, J. Comput. Chem..
[28] M. Levitt,et al. Theoretical studies of enzymic reactions: dielectric, electrostatic and steric stabilization of the carbonium ion in the reaction of lysozyme. , 1976, Journal of molecular biology.
[29] G. Ciccotti,et al. Numerical Integration of the Cartesian Equations of Motion of a System with Constraints: Molecular Dynamics of n-Alkanes , 1977 .
[30] Hoover,et al. Canonical dynamics: Equilibrium phase-space distributions. , 1985, Physical review. A, General physics.
[31] Alexander D. MacKerell,et al. Balancing the Interactions of Ions, Water, and DNA in the Drude Polarizable Force Field , 2014, The journal of physical chemistry. B.
[32] Alexander D. MacKerell,et al. Differential Impact of the Monovalent Ions Li+, Na+, K+, and Rb+ on DNA Conformational Properties , 2014, The journal of physical chemistry letters.
[33] W. L. Jorgensen,et al. Comparison of simple potential functions for simulating liquid water , 1983 .
[34] Jianpeng Ma,et al. CHARMM: The biomolecular simulation program , 2009, J. Comput. Chem..
[35] C. R. Mann. The Theory of Optics , 1903, Nature.
[36] B. Berne,et al. Combined fluctuating charge and polarizable dipole models: Application to a five-site water potential function , 2001 .
[37] Bruce J. Berne,et al. Dynamical Fluctuating Charge Force Fields: The Aqueous Solvation of Amides , 1996 .
[38] Alexander D. MacKerell,et al. Polarizable Empirical Force Field for Hexopyranose Monosaccharides Based on the Classical Drude Oscillator , 2014, The journal of physical chemistry. B.
[39] T. Darden,et al. A smooth particle mesh Ewald method , 1995 .
[40] Carsten Kutzner,et al. GROMACS 4: Algorithms for Highly Efficient, Load-Balanced, and Scalable Molecular Simulation. , 2008, Journal of chemical theory and computation.
[41] P. Kollman,et al. Settle: An analytical version of the SHAKE and RATTLE algorithm for rigid water models , 1992 .
[42] Steven J. Stuart,et al. Dynamical fluctuating charge force fields: Application to liquid water , 1994 .
[43] Alexander D. MacKerell,et al. Induction of peptide bond dipoles drives cooperative helix formation in the (AAQAA)3 peptide. , 2014, Biophysical journal.
[44] S. Nosé. A unified formulation of the constant temperature molecular dynamics methods , 1984 .
[45] Alexander D. MacKerell,et al. Recent Advances in Polarizable Force Fields for Macromolecules: Microsecond Simulations of Proteins Using the Classical Drude Oscillator Model , 2014, The journal of physical chemistry letters.
[46] Alexander D. MacKerell,et al. Development of a polarizable intermolecular potential function (PIPF) for liquid amides and alkanes. , 2007, Journal of chemical theory and computation.
[47] Mark E. Tuckerman,et al. Explicit reversible integrators for extended systems dynamics , 1996 .
[48] Benoît Roux,et al. Atomic Level Anisotropy in the Electrostatic Modeling of Lone Pairs for a Polarizable Force Field Based on the Classical Drude Oscillator. , 2006, Journal of chemical theory and computation.
[49] Alexander D. MacKerell,et al. A polarizable model of water for molecular dynamics simulations of biomolecules , 2006 .
[50] Alexander D. MacKerell,et al. Simulating Monovalent and Divalent Ions in Aqueous Solution Using a Drude Polarizable Force Field. , 2010, Journal of chemical theory and computation.