Banchmark: DeltaCodesDFT ¶

Codes precision measured using the database of bulk systems from https://molmod.ugent.be/DeltaCodesDFT. See the project page for details.

Key-value pairs ¶

key	description
kptdensity	K-point density in point per Ang^-1
linspacestr	Numpy’s linspace used for scaling the cell along the EOS
name	Name of the elemental bulk system (H-Ba, Lu-Po, Rn)
project	Name of the project: “dcdft”
width	Electronic temperature
x	Strain used to scale the cell along the EOS (see linspacestr)

Note that there are additional keys not explained above which are specific to the given calculator.

GPAW results for PAW datasets version 0.9 ¶

Running the following script writes the EOS parameters: V0 in Å**3/atom, bulk modulus (B0) in GPa, and pressure derivative of the bulk modulus B1 (dimensionless), in a file format expected by the calcDelta.py script available from https://molmod.ugent.be/DeltaCodesDFT

import sys
import numpy as np
from numpy.linalg.linalg import LinAlgError
from ase.units import kJ
import ase.db
from ase.utils import prnt
from ase.test.tasks.dcdft import DeltaCodesDFTCollection as Collection
from ase.test.tasks.dcdft import FullEquationOfState as EquationOfState

collection = Collection()

if len(sys.argv) == 2 and 'run.py' not in sys.argv:
    db = sys.argv[1]
else:
    db = 'dcdft_gpaw_pw_paw09.db'  # default db file

c = ase.db.connect(db)


def analyse(c, collection):

    A = []
    for name in collection.names:
        ve = []  # volume, energy pairs
        for row in c.select(name=name):
            try:
                ve.append((abs(np.linalg.det(row.cell)), row.energy))
            except AttributeError:
                ve.append((np.nan, np.nan))

        # sort according to volume
        ves = sorted(ve, key=lambda x: x[0])

        # EOS
        eos = EquationOfState([t[0] for t in ves], [t[1] for t in ves])
        try:
            v, e, B0, B1, R = eos.fit()
        except (ValueError, TypeError, LinAlgError):
            (v, e, B0, B1, R) = (np.nan, np.nan, np.nan, np.nan, np.nan)
        if not R:
            R = [np.nan]  # sometimes R is an empty array
        if not isinstance(R, list):
            R = [R]  # sometimes R is not a list
        e = e / len(collection[name])
        v = v / len(collection[name])
        B0 = B0 / kJ * 1.0e24  # GPa
        A.append((e, v, B0, B1, R[0]))
    return np.array(A).T


E, V, B0, B1, R = analyse(c, collection)

fd = open(db + '_raw.txt', 'w')
for name, e, v, b0, b1, r, in zip(collection.names, E, V, B0, B1, R):
    if not np.isnan(e):
        prnt('%2s %8.4f %8.4f %8.4f' % (name, v, b0, b1), file=fd)
fd = open(db + '_raw.csv', 'w')
for name, e, v, b0, b1, r, in zip(collection.names, E, V, B0, B1, R):
    if not np.isnan(e):
        prnt('%s, %8.4f, %8.4f, %8.4f' % (name, v, b0, b1), file=fd)

Results from other codes ¶

Consists of two steps. First extract the data for the given code and insert it into a new database file. Then use the extract.py script above to write the formatted file using the data from the new database file.

# aims light basis relativistic atomic_zora scalar
ase-db dcdft.db project=dcdft,calculator=aims,basis=light,relativistic=scalar -i dcdft_aims_light.db
python extract.py dcdft_aims_light.db
# aims tight basis relativistic atomic_zora scalar
ase-db dcdft.db project=dcdft,calculator=aims,basis=tight,relativistic=scalar -i dcdft_aims_tight.db
python extract.py dcdft_aims_tight.db
# aims really_tight basis relativistic atomic_zora scalar
ase-db dcdft.db project=dcdft,calculator=aims,basis=really_tight,relativistic=scalar -i dcdft_aims_really_tight.db
python extract.py dcdft_aims_really_tight.db
# aims tier2 basis relativistic atomic_zora scalar
ase-db dcdft.db project=dcdft,calculator=aims,basis=tier2,relativistic=scalar -i dcdft_aims_tier2.db
python extract.py dcdft_aims_tier2.db
# aims tier2 basis relativistic zora scalar 1e-12
ase-db dcdft.db project=dcdft,calculator=aims,basis=tier2,relativistic=1.e-12 -i dcdft_aims_tier2_z12.db
python extract.py dcdft_aims_tier2_z12.db
# aims tier2 basis relativistic none
ase-db dcdft.db project=dcdft,calculator=aims,basis=tier2,relativistic=none -i dcdft_aims_tier2_nrel.db
python extract.py dcdft_aims_tier2_nrel.db
# espresso gbrv 1.2
ase-db dcdft.db project=dcdft,calculator=espresso,potentials=gbrv,potentials_version=1.2 -i dcdft_espresso_gbrv_1.2.db
python extract.py dcdft_espresso_gbrv_1.2.db
# espresso gbrv 1.4
ase-db dcdft.db project=dcdft,calculator=espresso,potentials=gbrv,potentials_version=1.4 -i dcdft_espresso_gbrv_1.4.db
python extract.py dcdft_espresso_gbrv_1.4.db
# espresso sg15_oncv
ase-db dcdft.db project=dcdft,calculator=espresso,potentials=sg15_oncv -i dcdft_espresso_sg15_oncv.db
python extract.py dcdft_espresso_sg15_oncv.db
# espresso sssp_accuracy
ase-db dcdft.db project=dcdft,calculator=espresso,potentials=sssp_accuracy -i dcdft_espresso_sssp_accuracy.db
python extract.py dcdft_espresso_sssp_accuracy.db
# abinit gbrv
ase-db dcdft.db project=dcdft,calculator=abinit,potentials=gbrv -i dcdft_abinit_gbrv.db
python extract.py dcdft_abinit_gbrv.db
# abinit hgh
ase-db dcdft.db project=dcdft,calculator=abinit,potentials=hgh -i dcdft_abinit_hgh.db
python extract.py dcdft_abinit_hgh.db
# abinit hgh.sc
ase-db dcdft.db project=dcdft,calculator=abinit,potentials=hgh.sc -i dcdft_abinit_hgh_sc.db
python extract.py dcdft_abinit_hgh_sc.db
# abinit jth
ase-db dcdft.db project=dcdft,calculator=abinit,potentials=jth -i dcdft_abinit_jth.db
python extract.py dcdft_abinit_jth.db
# abinit paw
ase-db dcdft.db project=dcdft,calculator=abinit,potentials=gpaw -i dcdft_abinit_paw09.db
python extract.py dcdft_abinit_paw09.db
# gpaw paw grid spacing 0.10 Angstrom, number of grid points fixed
ase-db dcdft.db project=dcdft,calculator=gpaw,mode=fd,e=0.10,potentials_version=09 -i dcdft_gpaw_fd10_paw09.db
python extract.py dcdft_gpaw_fd10_paw09.db
# gpaw paw grid spacing 0.08 Angstrom, number of grid points fixed
ase-db dcdft.db project=dcdft,calculator=gpaw,mode=fd,e=0.08,potentials_version=09 -i dcdft_gpaw_fd_paw09.db
python extract.py dcdft_gpaw_fd_paw09.db
# gpaw paw planewave cutoff 100 Rydberg, number of grid points and planewaves variable
ase-db dcdft.db project=dcdft,calculator=gpaw,mode=pw,e=1361.0,constant_basis=0,potentials_version=09 -i dcdft_gpaw_pw_variable_paw09.db
python extract.py dcdft_gpaw_pw_variable_paw09.db
# gpaw paw planewave cutoff 100 Rydberg, number of grid points and planewaves fixed
ase-db dcdft.db project=dcdft,calculator=gpaw,mode=pw,e=1361.0,constant_basis=1,potentials_version=09 -i dcdft_gpaw_pw_paw09.db
python extract.py dcdft_gpaw_pw_paw09.db

A typical example of analysing data could be a verification of the results stored https://molmod.ugent.be/DeltaCodesDFT against the database.

cd /tmp
svn co https://svn.fysik.dtu.dk/projects/ase/trunk ase
cd ase
wget https://cmr.fysik.dtu.dk/_downloads/dcdft.db
PYTHONPATH=.:$PYTHONPATH PATH=tools:$PATH ase-db dcdft.db calculator=aims,basis=tight,relativistic=scalar -i dcdft_aims_tight.db
wget https://svn.fysik.dtu.dk/projects/cmr2/trunk/dcdft/extract.py
python extract.py dcdft_aims_tight.db
wget https://molmod.ugent.be/sites/default/files/Delta_v3-0.zip
unzip -p Delta_v3-0.zip  history.tar.gz > history.tar.gz
tar zxf history.tar.gz
sed '1,/with tight/d;/with light/,$d'  history/AIMS-history.txt > web.txt
diff -w web.txt dcdft_aims_tight.db_raw.txt

Running the calculations again ¶

Selected scripts used to obtain the results are available at https://gpaw.readthedocs.io/setups/dcdft.html

Banchmark: DeltaCodesDFT ¶

Key-value pairs ¶

GPAW results for PAW datasets version 0.9 ¶

Results from other codes ¶

Running the calculations again ¶

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Banchmark: DeltaCodesDFT¶

Key-value pairs¶

GPAW results for PAW datasets version 0.9¶

Results from other codes¶

Running the calculations again¶

Banchmark: DeltaCodesDFT ¶

Key-value pairs ¶

GPAW results for PAW datasets version 0.9 ¶

Results from other codes ¶

Running the calculations again ¶