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Third round of examples clean-up (i-pi#278)
incomplete work towards these goals * use lowercase names rather than Camel_Case * use underscores rather than hyphen consistently * flatten a bit the folder hierarchy - all the feature_type/feature/lammps_something should be just feature_type/feature * use driver whenever possible --------- Co-authored-by: litman90 <[email protected]>
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examples/features/Classical_molecular_dynamics/NVT_ensemble/lammps_h2o_liquid_water/in.lmp
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examples/features/Geometry_optimization/Nudge_elastic_band/zundel/h5o2.dms4B.coeff.com.dat
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examples/features/Geometry_optimization/Nudge_elastic_band/zundel/h5o2.pes4B.coeff.dat
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examples/features/Path_integral_quantum_dynamics/TRPMD/lammps_h2o_liquid_water/data.lmp
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examples/features/Path_integral_quantum_dynamics/TRPMD/lammps_h2o_liquid_water/water_216.xyz
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examples/features/Vibrations/harmonic/eNMFD-NormalModes/lammps_h2o-molecule/run.sh
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...es/Classical_molecular_dynamics/README.md → ...es/classical_molecular_dynamics/README.md
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Classical molecular dynamics. | ||
================================================= | ||
NVT_ensemble: global thermostatted classical NVT simulations | ||
nvt_ensemble: global thermostatted classical NVT simulations | ||
NPzT_ensemble_BZP: classical NVT simulations with the BZP barostat with only the z-component cell allowed to fluctuate | ||
NPzT_ensemble_MTTK: classical NVT simulations with the MTTK barostat with only the z-component cell allowed to fluctuate |
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examples/features/classical_molecular_dynamics/nvt_ensemble/run.sh
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ipi=i-pi | ||
driver="i-pi-driver -m qtip4pf -u -a h2o-md.1" | ||
sleep_time=4 | ||
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${ipi} input.xml > log.i-pi & | ||
echo "# i-PI is running" | ||
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echo "# Waiting for ${sleep_time} (s) before executing driver" | ||
sleep ${sleep_time} | ||
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${driver} > /dev/null & | ||
echo "# Driver is running" | ||
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wait | ||
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echo "# Simulation complete" |
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examples/features/classical_molecular_dynamics/nvt_ensemble/water_216.xyz
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../../../init_files/water_216.xyz |
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Metadynamics calculations using PLUMED | ||
====================================== | ||
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There are three examples of different variations-on-a-theme of the use of `<ffplumed>` | ||
to perform metadynamics calculations with i-PI | ||
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`pimd_metadynamics` : metadynamics using a centroid bias for a PIMD calculation | ||
`wte_metadynamics` : well-tempered ensemble. requires a workaround to communicate the energy as a CV | ||
`remd_metadynamics` : replica exchange combined with metadynamics | ||
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These examples can be run using the Zundel PES implemented in the i-pi driver, | ||
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```bash | ||
i-pi--driver -u -h zundel -m zundel | ||
``` | ||
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However, they require having PLUMED libraries and Python bindings in the appropriate system paths. |
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examples/features/metadynamics/wte_metadynamics/h5o2.dms4B.coeff.com.dat
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../../../../drivers/f90/pes/h5o2.dms4B.coeff.com.dat |
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examples/features/metadynamics/wte_metadynamics/h5o2.pes4B.coeff.dat
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../../../../drivers/f90/pes/h5o2.pes4B.coeff.dat |
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Open path integral calculations for momentum distribution. | ||
================================================= | ||
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`water_onepath`: An open-path integral calculation with one atom represented with an open path while all others are represented with a closed path. This setup can be used for rigorous estimation of the momentum distribution of a particle. | ||
`one_path`: An open-path integral calculation with one atom represented with an open path while all others are represented with a closed path. This setup can be used for rigorous estimation of the momentum distribution of a particle. | ||
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`water_multipath`: An open-path integral calculation with multiple atoms of a single atom type are represented with an open path while all others are represented with a closed path. Practically, this allows to average the momentum distribution over multiple atoms but it is not a rigorous way to estimate the momentum distribution of an atom if the kinetic energies of the different atoms are correlated. | ||
`multi_path`: An open-path integral calculation with multiple atoms of a single atom type are represented with an open path while all others are represented with a closed path. Practically, this allows to average the momentum distribution over multiple atoms but it is not a rigorous way to estimate the momentum distribution of an atom if the kinetic energies of the different atoms are correlated. |
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