Exploring canyons in glassy energy landscapes using metadynamics
暂无分享,去创建一个
[1] Pulin Gong,et al. Anomalous diffusion dynamics of learning in deep neural networks , 2020, Neural Networks.
[2] P. Wolynes,et al. Glass Dynamics Deep in the Energy Landscape. , 2021, The journal of physical chemistry. B.
[3] L. Berthier,et al. Stable glassy configurations of the Kob-Andersen model using swap Monte Carlo. , 2020, The Journal of chemical physics.
[4] David J Wales,et al. Exploring Energy Landscapes. , 2018, Annual review of physical chemistry.
[5] J. Russo,et al. The race to the bottom: approaching the ideal glass? , 2017, Journal of physics. Condensed matter : an Institute of Physics journal.
[6] L. Berthier,et al. Exploring the jamming transition over a wide range of critical densities , 2017, 1705.10156.
[7] L. Berthier,et al. Configurational entropy measurements in extremely supercooled liquids that break the glass ceiling , 2017, Proceedings of the National Academy of Sciences.
[8] Robert A. Riggleman,et al. Understanding soft glassy materials using an energy landscape approach. , 2016, Nature materials.
[9] T. Speck,et al. Non-Equilibrium Phase Transition in an Atomistic Glassformer: the Connection to Thermodynamics , 2016, 1603.06892.
[10] Ludovic Berthier,et al. Equilibrium Sampling of Hard Spheres up to the Jamming Density and Beyond. , 2015, Physical review letters.
[11] G. Meera Gandhi,et al. Cluster Based Outlier Detection Algorithm for Healthcare Data , 2015 .
[12] Philip Ball,et al. The hidden structure of liquids. , 2014, Nature materials.
[13] Giorgio Parisi,et al. Fractal free energy landscapes in structural glasses , 2014, Nature Communications.
[14] A. Stukowski. Structure identification methods for atomistic simulations of crystalline materials , 2012, 1202.5005.
[15] Peter Sollich,et al. Thermodynamic interpretation of soft glassy rheology models. , 2012, Physical review. E, Statistical, nonlinear, and soft matter physics.
[16] C. O’Hern,et al. Calculations of the structure of basin volumes for mechanically stable packings. , 2011, Physical review. E, Statistical, nonlinear, and soft matter physics.
[17] L. Berthier. Dynamic heterogeneity in amorphous materials , 2011, 1106.1739.
[18] Daan Frenkel,et al. Direct determination of the size of basins of attraction of jammed solids. , 2011, Physical review letters.
[19] Andrea J. Liu,et al. The Jamming Transition and the Marginally Jammed Solid , 2010 .
[20] Sidney Yip,et al. Computing the viscosity of supercooled liquids. , 2009, The Journal of chemical physics.
[21] Kenneth W. Desmond,et al. Random close packing of disks and spheres in confined geometries. , 2009, Physical review. E, Statistical, nonlinear, and soft matter physics.
[22] A. Stukowski. Visualization and analysis of atomistic simulation data with OVITO–the Open Visualization Tool , 2009 .
[23] Paul N. Mortenson,et al. Energy landscapes: from clusters to biomolecules , 2007 .
[24] J. Doye,et al. Power-law distributions for the areas of the basins of attraction on a potential energy landscape. , 2005, Physical review. E, Statistical, nonlinear, and soft matter physics.
[25] Pekka Koskinen,et al. Structural relaxation made simple. , 2006, Physical review letters.
[26] C. O’Hern,et al. Random close packing revisited: ways to pack frictionless disks. , 2005, Physical review. E, Statistical, nonlinear, and soft matter physics.
[27] A. Laio,et al. Escaping free-energy minima , 2002, Proceedings of the National Academy of Sciences of the United States of America.
[28] David J. Wales,et al. Crystals of binary Lennard-Jones solids , 2001 .
[29] D. Wales,et al. Energy landscapes of some model glass formers , 2001 .
[30] Pablo G. Debenedetti,et al. Supercooled liquids and the glass transition , 2001, Nature.
[31] B. Richards,et al. Simple glass-forming liquids: their definition, fragilities, and landscape excitation profiles , 1999 .
[32] Lindsey J. Munro,et al. DEFECT MIGRATION IN CRYSTALLINE SILICON , 1999 .
[33] Srikanth Sastry,et al. Signatures of distinct dynamical regimes in the energy landscape of a glass-forming liquid , 1998, Nature.
[34] Peter Sollich. Rheological constitutive equation for a model of soft glassy materials , 1997, cond-mat/9712001.
[35] U. Hansmann. Parallel tempering algorithm for conformational studies of biological molecules , 1997, physics/9710041.
[36] J. Doye,et al. Global Optimization by Basin-Hopping and the Lowest Energy Structures of Lennard-Jones Clusters Containing up to 110 Atoms , 1997, cond-mat/9803344.
[37] Peter Sollich,et al. Rheology of Soft Glassy Materials , 1996, cond-mat/9611228.
[38] H. C. Andersen,et al. Testing mode-coupling theory for a supercooled binary Lennard-Jones mixture I: The van Hove correlation function. , 1995, Physical review. E, Statistical physics, plasmas, fluids, and related interdisciplinary topics.
[39] P. Grassberger,et al. Characterization of Strange Attractors , 1983 .
[40] W. Miller,et al. ON FINDING TRANSITION STATES , 1981 .
[41] Joseph Ford,et al. Numerical Experiments on the Stochastic Behavior of a Lennard-Jones Gas System , 1973 .
[42] J. Gower,et al. Minimum Spanning Trees and Single Linkage Cluster Analysis , 1969 .