Source code for mppi.Parsers.PwParser

"""
Class to perform the parsing of a QuantumESPRESSO XML file. Makes usage of the
data-file-schema.xml file that is found in the run_dir/prefix.save folder.
"""

from mppi.Utilities.Constants import HaToeV
from mppi.Parsers import ParsersUtils as U
from mppi.Utilities import LatticeUtils as latUtils

[docs]class PwParser(): """ Initialize the data member of the class. Args: file (str): The name, including the path of the data-file-schema.xml verbose (bool) : set the amount of information written on terminal Attributes: natoms : number of atoms in the cell natypes : number of atomic species atomic_positions : list with the name and position of each atom, expressed in cartesian coordinates (in a.u.) atomic_species : dictionary with mass and pseudo for each species alat : lattice parameter (in a.u.) lattice : array with the lattice vector. The i-th row represents the i-th lattice vectors in cartesian units syms : list with the symmetries of the lattice num_electrons : number of electrons nkpoints : numer of kpoints nbands : number of bands nbands_full : number of occupied bands (for systems with a gap) nbands_empty : number of empty bands (for systems with a gap) occupations_kind : type of occupation (fixed or smearing) kpoints : array with the kpoints occupations : array with the bands occupation for each kpoint weights : array with the weight of each kpoint, each element is a one-dimensional array. energy : total energy of the system (in Hartree) evals : array of the ks energies for each kpoint (in Hartree) lsda : True if collinear spin is activated noncolin : True if noncollinear spin calculation is activated spinorbit : True if spin-orbit couping is present spin_degen : 1 if lsda or non collinear spin is activated, 2 otherwise """ def __init__(self,file,verbose=True): self.file = file if verbose: print('Parse file : %s'%self.file) try: self.parseXML(self.file) except TypeError: #FileNotFoundError or TypeError: if verbose: print('Failed to read %s'%self.file) self.data = None
[docs] def parseXML(self,file): """ Read the data from the xml file in the new format of QuantumESPRESSO. Some variable are extracted from the XML file and stored in the attributes of the object. """ import xml.etree.ElementTree as ET import numpy as np self.data = ET.parse(file).getroot() # Add some relevant attributes to the object #units used in the XML data file self.units = self.data.attrib['Units'] #atomic number and positions self.natoms = int(self.data.find("output/atomic_structure").get('nat')) self.atomic_positions = [] atoms = self.data.findall("output/atomic_structure/atomic_positions/atom") for i in range(self.natoms): atype = atoms[i].get('name') pos = [float(x) for x in atoms[i].text.strip().split()] self.atomic_positions.append([atype,np.array(pos)]) #atomic species self.natypes = int(self.data.find("output/atomic_species").get('ntyp')) atypes = self.data.findall("output/atomic_species/species") self.atomic_species = {} for i in range(self.natypes): atype_string = atypes[i].get('name') atype_mass = atypes[i].findall('mass')[0].text atype_pseudo = atypes[i].findall('pseudo_file')[0].text self.atomic_species[atype_string]=[atype_mass,atype_pseudo] #lattice properties self.alat = float(self.data.find("output/atomic_structure").get('alat')) lattice = [] for i in [1,2,3]: lat_vect = self.data.findall("output/atomic_structure/cell/a%d"%i)[0] lat_vect = [float(x) for x in lat_vect.text.strip().split()] lattice.append(lat_vect) self.lattice = np.array(lattice) symmetries = self.data.findall('output/symmetries/symmetry') self.syms = [] for sym in symmetries: rotation = [float(x) for x in sym.find('rotation').text.split()] self.syms.append(np.array(rotation).reshape(3,3)) #number of electrons self.num_electrons = float(self.data.find('output/band_structure/nelec').text) #number of kpoints and bands self.nkpoints = int(self.data.find('output/band_structure/nks').text) self.nbands = int(self.data.find('output/band_structure/nbnd').text) #spin related properties and spin-orbit coupling lsda = self.data.find('output/band_structure/lsda').text self.lsda = True if lsda == 'true' else False noncolin = self.data.find('output/band_structure/noncolin').text self.noncolin = True if noncolin == 'true' else False spinorbit = self.data.find('output/band_structure/spinorbit').text self.spinorbit = True if spinorbit == 'true' else False self.spin_degen = 1 if self.lsda or self.noncolin else 2 #number of occupied and empty bands (for systems with a gap) self.nbands_full = int(self.num_electrons/self.spin_degen) self.nbands_empty = self.nbands-self.nbands_full #total energy self.energy = float(self.data.find('output/total_energy/etot').text) #occupations kind (fixed or smearing) self.occupations_kind = self.data.find('output/band_structure/occupations_kind').text kstates = self.data.findall('output/band_structure/ks_energies') #arrays with the kpoints, the associated weights, the ks energies and the occupations self.kpoints = [] self.weights = [] self.evals = [] self.occupations = [] for k in kstates: kpoint = [float(x) for x in k.find('k_point').text.split()] weight = [float(x) for x in k.find('k_point').get('weight').split()] eval = [float(x) for x in k.find('eigenvalues').text.split()] occ = [float(x) for x in k.find('occupations').text.split()] self.kpoints.append(kpoint) self.weights.append(weight) self.evals.append(eval) self.occupations.append(occ) self.kpoints = np.array(self.kpoints) self.weights = np.array(self.weights) self.evals = np.array(self.evals) self.occupations = np.array(self.occupations)
[docs] def get_energy(self,convert_eV = True): """ Return the total energy the system. If convert_eV is True the energy is provided in eV other the Hartree units are used. """ if convert_eV: return HaToeV*self.energy else: return self.energy
[docs] def get_fermi(self,convert_eV = True): """ Return the fermi energy of the system (if present in the xml file). If convert_eV is True the fermi energy is provided in eV, otherwise the Hartree units are used. """ fermi = self.data.find('output/band_structure/fermi_energy') if fermi is not None: fermi = float(fermi.text) if convert_eV: fermi *= HaToeV return fermi else: print('Fermi energy attribute not found in the ouput file. Maybe `fixed` occupation type is used?') return None
[docs] def eval_lattice_volume(self, rescale = False): """ Compute the volume of the direct lattice. If ``rescale`` is False the results is expressed in a.u., otherwise the lattice vectors are expressed in units of alat. Returns: :py:class:`float` : lattice volume """ lattice = self.get_lattice(rescale=rescale) return latUtils.eval_lattice_volume(lattice)
[docs] def eval_reciprocal_lattice_volume(self, rescale = False): """ Compute the volume of the reciprocal lattice. If ``rescale`` is True the reciprocal lattice vectors are expressed in units of 2*np.pi/alat. Returns: :py:class:`float` : reciprocal lattice volume """ lattice = self.get_reciprocal_lattice(rescale=rescale) return latUtils.eval_lattice_volume(lattice)
[docs] def get_lattice(self, rescale = False): """ Compute the lattice vectors. If rescale = True the vectors are expressed in units of the lattice constant. Args: rescale (:py:class:`bool`) : if True express the lattice vectors in units alat Returns: :py:class:`array` : array with the lattice vectors a_i as rows """ return latUtils.get_lattice(self.lattice,self.alat,rescale=rescale)
[docs] def get_reciprocal_lattice(self, rescale = False): """ Compute the reciprocal lattice vectors. If rescale = False the vectors are normalized so that np.dot(a_i,b_j) = 2*np.pi*delta_ij, where a_i is a basis vector of the direct lattice. If rescale = True the reciprocal lattice vectors are expressed in units of 2*np.pi/alat. Args: rescale (:py:class:`bool`) : if True express the reciprocal vectors in units of 2*np.pi/alat Returns: :py:class:`array` : array with the reciprocal lattice vectors b_i as rows """ return latUtils.get_reciprocal_lattice(self.lattice,self.alat,rescale=rescale)
[docs] def get_evals(self, set_scissor = None, set_gap = None, set_direct_gap = None, verbose = True): """ Return the ks energies for each kpoint (in eV). The top of the valence band is used as the reference energy value. It is possible to shift the energies of the empty bands by setting an arbitrary value for the gap (direct or indirect) or by adding an explicit scissor. Implemented only for semiconductors, the energy shift of empty bands does not update their occupation levels. Args: set_scissor (:py:class:`float`) : set the value of the scissor (in eV) that is added to the empty bands. If a scissor is provided the set_gap and set_direct_gap parameters are ignored set_gap (:py:class:`float`) : set the value of the gap (in eV) of the system. If set_gap is provided the set_direct_gap parameter is ignored set_direct_gap (:py:class:`float`) : set the value of the direct gap (in eV) of the system. Return: :py:class:`numpy.array` : an array with the ks energies for each kpoint """ evals = U.get_evals(self.evals,self.nbands,self.nbands_full, set_scissor=set_scissor,set_gap=set_gap,set_direct_gap=set_direct_gap,verbose=verbose) return evals
[docs] def get_transitions(self, initial = 'full', final = 'empty',set_scissor = None, set_gap = None, set_direct_gap = None): """ Compute the (vertical) transitions energies. For each kpoint compute the transition energies, i.e. the (positive) energy difference (in eV) between the final and the initial states. Args: initial (string or list) : specifies the bands from which electrons can be extracted. It can be set to `full` or `empty` to select the occupied or empty bands, respectively. Otherwise a list of bands can be provided final (string or list) : specifies the final bands of the excited electrons. It can be set to `full` or `empty` to select the occupied or empty bands, respectively. Otherwise a list of bands can be provided set_scissor (:py:class:`float`) : set the value of the scissor (in eV) that is added to the empty bands. If a scissor is provided the set_gap and set_direct_gap parameters are ignored set_gap (:py:class:`float`) : set the value of the gap (in eV) of the system. If set_gap is provided the set_direct_gap parameter is ignored set_direct_gap (:py:class:`float`) : set the value of the direct gap (in eV) of the system. Return: :py:class:`numpy.array` : an array with the transition energies for each kpoint """ transitions = U.get_transitions(self.evals,self.nbands,self.nbands_full,initial=initial,final=final, set_scissor=set_scissor,set_gap=set_gap,set_direct_gap=set_direct_gap) return transitions
[docs] def get_gap(self, verbose = True): """ Compute the energy gap of the system (in eV). The method check if the gap is direct or indirect. Implemented and tested only for semiconductors. Return: :py:class:`dict` : a dictionary with the values of direct and indirect gaps and the positions of the VMB and CBM """ gap = U.get_gap(self.evals,self.nbands_full,verbose=verbose) return gap