Source code for ase2sprkkr.output_files.definitions.spc

from ..output_files_definitions import OutputFileValueDefinition as V, create_output_file_definition, OutputFileDefinition
from typing import Optional
import numpy as np

from ..output_files import Arithmetic, CommonOutputFile
from ...common.grammar_types import NumpyArray, Prefixed
from ...common.generated_configuration_definitions import NumpyViewDefinition as NV, \
                                                          GeneratedValueDefinition as GV
from ...common.configuration_definitions import switch
from ...gui.plot import change_default_kwargs, colormesh, Multiplot
import matplotlib.pyplot as plt


[docs] class ARPESOutputFile(CommonOutputFile, Arithmetic):
[docs] def plot(self, layout=(2,2), figsize=(10,6), latex=None, filename:Optional[str]=None, show:Optional[bool]=None, dpi=800, separate_plots=False, **kwargs ): with Multiplot(layout=layout, figsize=figsize, latex=latex, filename=filename, show=show, dpi=dpi, separate_plots=separate_plots, **kwargs) as mp: mp.plot(self.TOTAL) mp.plot(self.UP) mp.plot(self.DOWN) mp.plot(self.POLARIZATION)
[docs] def _arithmetic_values(self): return [('RAW_DATA', (slice(None), slice(2, 6 if self.MODE() == 'energy' else 5)))]
[docs] def _assert_arithmetic(self, other): """ Check, that the file can be summed/subtracked from an other file """ assert self.MODE() == other.MODE() if self.MODE() == 'energy': assert np.allclose(other.ENERGY(), self.ENERGY()) assert np.allclose(other.THETA(), self.THETA()) else: assert np.allclose(other.KX(), self.KX()) assert np.allclose(other.KY(), self.KY())
[docs] class ARPESDefinition(OutputFileDefinition): result_class = ARPESOutputFile
[docs] def create_definition(): def plot(option, **kwargs): c = option._container kw = { 'show_zero_line' : False, 'mode' : 'from_zero', 'norm' : 'log', 'vmax': np.max([c.TOTAL().max(), c.UP().max(), c.DOWN().max()]), } if c.MODE() == 'energy': x = c.THETA() y = c.ENERGY() kw['xlabel'] = r'$\theta$ (deg)' kw['ylabel'] = r'$E-E_{\rm F}$ (eV)' else: x = c.KX() y = c.KY() kw['xlabel'] = r'$k_x$ (Å$^{-1}$)' kw['ylabel'] = r'$k_y$ (Å$^{-1}$)' kw.update(kwargs) colormesh(x, y, option(), **kw) def i(j): return slice(None),j def determinant(data, c): if c.MODE() == 'energy': return data[:,7].reshape(c.NE(), c.NT()) return data[:,6].reshape(c.NE(), c.NT()) def ii(j): def fn(data, c): first = c.NE if c.MODE() == 'energy' else c.NP return data[:,j].reshape(first(), c.NT()) return fn definition = create_output_file_definition('ARPES', [ V('NT', int), V('NP', int), V('COMMENT', Prefixed('#'), name_in_grammar=False), V('RAW_DATA', NumpyArray(written_shape=(-1,8)), name_in_grammar=False), GV('MODE', lambda c,k=None: 'energy' if c.NE() > 1 else 'kx_ky'), *switch('MODE', { 'energy': [ NV('THETA', 'RAW_DATA', i(0), ('NE', 'NT')), NV('ENERGY', 'RAW_DATA', i(1), ('NE', 'NT')), NV('K', 'RAW_DATA', i(6), ('NE', 'NT'), info='K_parallel (pi/A)'), ], 'kx_ky': [ NV('KX', 'RAW_DATA', i(0), ('NP', 'NT'), info='k_x coordinate (1/Å)'), NV('KY', 'RAW_DATA', i(1), ('NP', 'NT'), info='k_y coordinate (1/Å)'), ] }), NV('TOTAL', 'RAW_DATA', ii(2), info='Total intensity', plot=change_default_kwargs(plot,title=r'Total intensity',colormap='gray')), NV('UP', 'RAW_DATA', ii(3), info='Spin up', plot=change_default_kwargs(plot,title=r'Spin up',colormap='gray')), NV('DOWN', 'RAW_DATA', ii(4), info='Spin down', plot=change_default_kwargs(plot, title=r'Spin down', colormap='gray')), NV('POLARIZATION', 'RAW_DATA', ii(5), info='Spin polarization', plot=change_default_kwargs(plot, colormap='bwr', title=r'Spin polarization') ), NV('DETERMINANT', 'RAW_DATA', determinant), ], cls=ARPESDefinition, info='ARPES (Angle-resolved photoemission spectroscopy) output (.spc file).') return definition
definition = create_definition()