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KIM Validation and Verification

Testing PyPI

This package allows the user to run any OpenKIM Test Drivers written using the kim-tools package locally. A "Test Driver" is a computational protocol that reports one or more material properties using the KIM Properties Framework

List of included Test Drivers:

  • EquilibriumCrystalStructure
  • ElasticConstantsCrystal
  • VacancyFormationEnergyRelaxationVolumeCrystal
  • HeatCapacityThermalExpansionCrystalNPT
  • GibbsFreeEnergyCrystal
  • CrystalStructureAndEnergyVsPressure
  • NPTCrystalStructure

To run one of these calculations, instantiate the class with an interatomic model, which can be a KIM potential installed on your system or an ASE Calculator (not all Test Drivers support ASE Calculators):

from kimvv import ElasticConstantsCrystal
elast = ElasticConstantsCrystal('LennardJones_Ar')

The object you instantiated can now be used to perform property calculations. You are required to provide a crystal structure, which can be specified as an ASE Atoms object (it is also possible to specify a symmetry-reduced crystallographic description, see examples below):

from ase.build import bulk
atoms = bulk('Ar')
results = elast(atoms)

Most Test Drivers accept other optional and/or required arguments. Use the printdoc method for an explanation of each Test Driver's operation, e.g. ElasticConstantsCrystal.printdoc(). Besides the structure, all Test Drivers accept the universal argument temperature_K, and the mutually exclusive pressure_eV_angstrom3 and cell_cauchy_stress_eV_angstrom3. These are ignored by Test Drivers that are restricted zero temperature and/or stress-free conditions.

It is *crucial* that you inspect the printdoc output for the calculation you plan to run. The defaults are chosen for maximum compatibility and accuracy, which means they are likely not practical. For example, the default settings for most finite temperature Test Drivers will attempt to run a 10,000 atom simulation as a serial LAMMPS job. See examples below for examples of practical input sets.

Installation

kimvv and all requirements are available in the KIM Developer Platform (KDP) container available here: https://github.com/openkim/developer-platform

kimvv is installable with pip install kimvv, but it requires some non-Python rquirements to be installed first. These prerequisites are decribed in installation info for kim-tools, the backend for kimvv, here: https://kim-tools.readthedocs.io/en/stable/#doc-standalone-installation.

Basic usage example:

Computing elastic constants for FCC argon using an example KIM potential

from kimvv import ElasticConstantsCrystal
from ase.build import bulk
from json import dumps

# The Test Driver must be instantiated with an ASE Calculator object
# or a string indicating a KIM model name
elast = ElasticConstantsCrystal('LennardJones_Ar')

# To perform the computation, call the Test Driver object. The first argument
# to most Test Drivers is the crystal structure to perform the computation on.
# To see an explanation of the calculation and a description of the
# additonal arguments, use .printdoc()
elast.printdoc()

# For the sake of speed, let's compute the elastic constants with the
# "stress-condensed" method, instead of the default robust computation loop.
# The crystal structure can be specified as an Atoms object. Any dependencies
# (e.g. relaxing the crystal structure with EquilibriumCrystalStructure) are
# automatically run.
atoms = bulk("Ar", "fcc", 5.0)
results = elast(atoms, method="stress-condensed")

# Each Test Driver computes a list of one or more dictionaries, each defining
# a material property in the format specified by the KIM Properties Framework.
# The name of the property is in the "property-id" key. See
# https://openkim.org/properties for the definition of each property.
print(dumps(results, indent=2))

Usage example 2

Computing heat capacity and thermal expansion coefficients of gold using an example KIM potential using a small system size running 3 LAMMPS processes using 2 CPUs each

from kimvv import HeatCapacityThermalExpansionCrystalNPT
from ase.build import bulk
atoms = bulk("Au")
td = HeatCapacityThermalExpansionCrystalNPT("Sim_LAMMPS_LJcut_AkersonElliott_Alchemy_PbAu")
result = td(atoms, temperature_K=300, target_size=1000, lammps_command="mpirun -np 2 --bind-to numa lmp", max_workers=3)

Usage example 3

Getting the anisotropic pressure-volume curve of HCP Ag using a non-KIM ASE Calculator

from kimvv import CrystalStructureAndEnergyVsPressure
from ase.build import bulk
from ase.calculators.emt import EMT

# The Test Driver must be instantiated with an ASE Calculator object
# or a string indicating a KIM model name
scan = CrystalStructureAndEnergyVsPressure(EMT())

# To perform the computation, call the Test Driver object. The first argument
# to most Test Drivers is the crystal structure to perform the compuation on.
# To see the additonal arguments, use .printdoc() to print the docstring
scan.printdoc()

# The default volume range of 0.25-4.0 will take a long time to scan. Let's
# do a much smaller range
results = scan(
    bulk("Ag", "hcp", 2.92), min_fractional_volume=0.98, max_fractional_volume=1.02
)

Usage example 4

This example is functionally identical to the previous example, except the crystal is specified by passing a dictionary specifying the symmetry-reduced description of the crystal

from kimvv import CrystalStructureAndEnergyVsPressure
from ase.calculators.emt import EMT

scan = CrystalStructureAndEnergyVsPressure(EMT())

# Specify the material using a symmetry-reduced dictionary.
# Internally, all kimvv Test Drivers use this representation,
# so this allows more direct control, as an Atoms object will
# be converted to this regardless. This allows you to specify
# the crystal in a specific orientation that will be maintained
# Notionally, this should be an instance of the
# `crystal-structure-npt` OpenKIM Property, but the exact schema
# is not enforced. As long as the following fields are present,
# it will work: "prototype-label.source-value",
# "stoichiometric-species.source-value", "a.source-value",
# and, if the crystal has any free parameters,
# "parameter-values.source-value".
# For an exact definition of these fields, see
# https://openkim.org/properties/show/crystal-structure-npt
# For more info about the AFLOW Prototype Designation,
# see section B here: https://arxiv.org/pdf/2401.06875
material = {
    "prototype-label": {"source-value": "A_hP2_194_c"},
    "stoichiometric-species": {"source-value": ["Ag"]},
    "a": {
        "source-value": 2.933,
        "source-unit": "angstrom",
    },
    "parameter-names": {"source-value": ["c/a"]},
    "parameter-values": {"source-value": [1.6373338]},
}


results = scan(material, min_fractional_volume=0.98, max_fractional_volume=1.02)
scan.write_property_instances_to_file("scan_output/results.edn")

Usage example 5

Querying for all DFT-relaxed structures for a given combination of elements in OpenKIM and relaxing them with your potential

from kimvv import EquilibriumCrystalStructure
from kim_tools import (
  query_crystal_structures,
  get_deduplicated_property_instances
)
from json import dumps
from ase.calculators.lj import LennardJones

# Query for all relaxed Argon reference data in OpenKIM
# You can narrow the query further by specifying more information
# about the crystal, see
# https://kim-tools.readthedocs.io/en/stable/kim_tools.test_driver.html#kim_tools.test_driver.core.query_crystal_structures
raw_structs = query_crystal_structures(stoichiometric_species=["Ar"])

# Deduplicate them
unique_structs = get_deduplicated_property_instances(raw_structs, allow_rotation=True)

# Instantiate the Driver with your model
relax = EquilibriumCrystalStructure(LennardJones(sigma=3.4,epsilon=0.0104,rc=8.15))

# Run the Driver with each structure. As this is run, the driver internally accumulates
# Property Instances
for struct in unique_structs:
  relax(struct)

# In addition to returning the Property Instances for the current run, Test Drivers
# accumulate all computed Property Instances. They can be accessed like this:
print(dumps(relax.property_instances, indent=2))

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