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starting examples
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jrudz committed Apr 9, 2024
1 parent 8399aa9 commit a282eb4
Showing 1 changed file with 106 additions and 78 deletions.
184 changes: 106 additions & 78 deletions src/nomad_simulations/outputs_JFR_temp.py
Original file line number Diff line number Diff line change
Expand Up @@ -1100,7 +1100,8 @@ def normalize(self, archive, logger) -> None:
super().normalize(archive, logger)
self.value_unit = 'pascal'
self.name = 'pressure_tensor'
self.variables = [['xx', 'xy', 'xz'], ['yx', 'yy', 'yz'], ['zx', 'zy', 'zz']]
self.bins = None
self.variables = [['x', 'y', 'z'], ['x', 'y', 'z']] # ? [['xx', 'xy', 'xz'], ['yx', 'yy', 'yz'], ['zx', 'zy', 'zz']]

class VirialTensor(TrajectoryOutputs):
"""
Expand All @@ -1118,7 +1119,7 @@ def normalize(self, archive, logger) -> None:
super().normalize(archive, logger)
self.value_unit = 'joule'
self.name = 'virial_tensor'
self.variables = [['xx', 'xy', 'xz'], ['yx', 'yy', 'yz'], ['zx', 'zy', 'zz']]
self.variables = [['x', 'y', 'z'], ['x', 'y', 'z']] # ? [['xx', 'xy', 'xz'], ['yx', 'yy', 'yz'], ['zx', 'zy', 'zz']]

class Temperature(TrajectoryOutputs):
"""
Expand All @@ -1136,16 +1137,115 @@ def normalize(self, archive, logger) -> None:
self.name = 'temperature'
self.is_scalar = True

class Volume(TrajectoryOutputs):
"""
Section containing the (scalar) temperature of a (sub)system.
"""

volume = Quantity(
type=np.dtype(np.float64),
shape=[],
value = Quantity(
type=np.float64,
unit='m ** 3',
)

def normalize(self, archive, logger) -> None:
super().normalize(archive, logger)
self.value_unit = 'm ** 3'
self.name = 'volume'
self.is_scalar = True

class Hessian(TrajectoryOutputs):
"""
Section containing the Hessian matrix, i.e., 2nd derivatives with respect to atomic displacements,
of the potential energy of a (sub)system.
"""

value = Quantity(
type=np.dtype(np.float64),
shape=['n_atoms', 'n_atoms', 3, 3],
unit='joule / m ** 2',
)

def normalize(self, archive, logger) -> None:
super().normalize(archive, logger)
self.value_unit = 'joule / m ** 2'
self.name = 'hessian'
self.variables = [['atom_index'], ['atom_index'], ['x', 'y', 'z'], ['x', 'y', 'z']]
self.bins = [np.range(self.n_atoms), np.range(self.n_atoms)]





class RadialDistributionFunction(TrajectoryOutputs):
"""
Section containing information about the calculation of
radial distribution functions (rdfs).
"""

value = Quantity(
type=np.dtype(np.float64),
shape=['*'],
)

variables = Quantity(
type=str,
shape=[1],
description="""
Value of the volume of the system at which the properties are calculated.
Name/description of the variables along which the property is defined.
""",
)

bins = Quantity(
type=np.float64,
shape=['*'],
unit='m',
description="""
Distances along which the rdf was calculated.
""",
)

def normalize(self, archive, logger):
super().normalize(archive, logger)
self.variables = ['distance']
assert len(self.bins) == len(self.value)


class Forces(TrajectoryOutputs):
"""
Section describing a contribution to or type of atomic forces.
"""

value = Quantity(
type=np.dtype(np.float64),
shape=['n_atoms', 3],
unit='newton',
description="""
Value of the forces acting on the atoms. This is calculated as minus gradient of
the corresponding energy type or contribution **including** constraints, if
present. The derivatives with respect to displacements of nuclei are evaluated in
Cartesian coordinates. In addition, these are obtained by filtering out the
unitary transformations (center-of-mass translations and rigid rotations for
non-periodic systems, see value_raw for the unfiltered counterpart).
""",
)

variables = Quantity(
type=str,
shape=['*'],
description="""
Name/description of the variables along which the property is defined.
""",
)

def normalize(self, archive, logger):
super().normalize(archive, logger)
self.bins = None
self.variables = ['atoms', 'x', 'y', 'z']
assert len(self.bins) == len(self.value)




heat_capacity_c_v = Quantity(
type=np.dtype(np.float64),
shape=[],
Expand Down Expand Up @@ -1228,82 +1328,10 @@ class BaseCalculation(ArchiveSection):
can be accessed in section workflow.
"""

m_def = Section(validate=False)

system_ref = Quantity(
type=Reference(System.m_def),
shape=[],
description="""
Links the calculation to a section system.
""",
categories=[FastAccess],
)

method_ref = Quantity(
type=Reference(Method.m_def),
shape=[],
description="""
Links the calculation to a section method.
""",
categories=[FastAccess],
)

starting_calculation_ref = Quantity(
type=Reference(SectionProxy('Calculation')),
shape=[],
description="""
Links the current section calculation to the starting calculation.
""",
categories=[FastAccess],
)

n_references = Quantity(
type=np.dtype(np.int32),
shape=[],
description="""
Number of references to the current section calculation.
""",
)

calculations_ref = Quantity(
type=Reference(SectionProxy('Calculation')),
shape=['n_references'],
description="""
Links the current section calculation to other section calculations. Such a link
is necessary for example if the referenced calculation is a self-consistent
calculation that serves as a starting point or a calculation is part of a domain
decomposed simulation that needs to be connected.
""",
categories=[FastAccess],
)

calculations_path = Quantity(
type=str,
shape=['n_references'],
description="""
Links the current section calculation to other section calculations. Such a link
is necessary for example if the referenced calculation is a self-consistent
calculation that serves as a starting point or a calculation is part of a domain
decomposed simulation that needs to be connected.
""",
)

calculation_converged = Quantity(
type=bool,
shape=[],
description="""
Indicates whether a the calculation is converged.
""",
)

hessian_matrix = Quantity(
type=np.dtype(np.float64),
shape=['number_of_atoms', 'number_of_atoms', 3, 3],
description="""
The matrix with the second derivative of the energy with respect to atom
displacements.
""",
)

spin_S2 = Quantity(
type=np.dtype(np.float64),
Expand Down

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