Source code for abipy.dynamics.hist

# coding: utf-8
"""History file with structural relaxation results."""
import os
import numpy as np
import pymatgen.core.units as units

from collections import OrderedDict
from monty.functools import lazy_property
from monty.collections import AttrDict
from monty.string import marquee, list_strings
from pymatgen.core.periodic_table import Element
from pymatgen.analysis.structure_analyzer import RelaxationAnalyzer
from abipy.tools.plotting import add_fig_kwargs, get_ax_fig_plt, get_axarray_fig_plt, set_visible, get_figs_plotly, \
    get_fig_plotly, add_plotly_fig_kwargs, plotlyfigs_to_browser, push_to_chart_studio, PlotlyRowColDesc, plotly_set_lims, \
    latex_greek_2unicode
from abipy.core.structure import Structure
from abipy.core.mixins import AbinitNcFile, NotebookWriter
from abipy.abio.robots import Robot
from abipy.iotools import ETSF_Reader
import abipy.core.abinit_units as abu


[docs]class HistFile(AbinitNcFile, NotebookWriter): """ File with the history of a structural relaxation or molecular dynamics calculation. Usage example: .. code-block:: python with HistFile("foo_HIST") as hist: hist.plot() .. rubric:: Inheritance Diagram .. inheritance-diagram:: HistFile """
[docs] @classmethod def from_file(cls, filepath): """Initialize the object from a netcdf_ file""" return cls(filepath)
def __init__(self, filepath): super().__init__(filepath) self.reader = HistReader(filepath)
[docs] def close(self): """Close the file.""" self.reader.close()
[docs] @lazy_property def params(self): """:class:`OrderedDict` with parameters that might be subject to convergence studies.""" return {}
def __str__(self): return self.to_string() # TODO: Add more metadata. #@lazy_property #def nsppol(self): # """Number of independent spins.""" # return self.reader.read_dimvalue("nsppol") #@lazy_property #def nspden(self): # """Number of independent spin densities.""" # return self.reader.read_dimvalue("nspden") #@lazy_property #def nspinor(self): # """Number of spinor components.""" # return self.reader.read_dimvalue("nspinor")
[docs] @lazy_property def final_energy(self): """Total energy in eV of the last iteration.""" return self.etotals[-1]
[docs] @lazy_property def final_pressure(self): """Final pressure in Gpa.""" cart_stress_tensors, pressures = self.reader.read_cart_stress_tensors() return pressures[-1]
#@lazy_property #def final_max_force(self):
[docs] def get_fstats_dict(self, step): """ Return |AttrDict| with stats on the forces at the given ``step``. """ # [time, natom, 3] var = self.reader.read_variable("fcart") forces = units.ArrayWithUnit(var[step], "Ha bohr^-1").to("eV ang^-1") fmods = np.array([np.linalg.norm(force) for force in forces]) return AttrDict( fmin=fmods.min(), fmax=fmods.max(), fmean=fmods.mean(), fstd=fmods.std(), drift=np.linalg.norm(forces.sum(axis=0)), )
[docs] def to_string(self, verbose=0, title=None): """String representation.""" lines = []; app = lines.append if title is not None: app(marquee(title, mark="=")) app(marquee("File Info", mark="=")) app(self.filestat(as_string=True)) app("") app(self.initial_structure.to_string(verbose=verbose, title="Initial Structure")) app("") app("Number of relaxation steps performed: %d" % self.num_steps) app(self.final_structure.to_string(verbose=verbose, title="Final structure")) app("") an = self.get_relaxation_analyzer() app("Volume change in percentage: %.2f%%" % (an.get_percentage_volume_change() * 100)) d = an.get_percentage_lattice_parameter_changes() vals = tuple(d[k] * 100 for k in ("a", "b", "c")) app("Percentage lattice parameter changes:\n\ta: %.2f%%, b: %.2f%%, c: %2.f%%" % vals) #an.get_percentage_bond_dist_changes(max_radius=3.0) app("") cart_stress_tensors, pressures = self.reader.read_cart_stress_tensors() app("Stress tensor (Cartesian coordinates in GPa):\n%s" % cart_stress_tensors[-1]) app("Pressure: %.3f [GPa]" % pressures[-1]) return "\n".join(lines)
@property def num_steps(self): """Number of iterations performed.""" return self.reader.num_steps
[docs] @lazy_property def steps(self): """Step indices.""" return list(range(self.num_steps))
@property def initial_structure(self): """The initial |Structure|.""" return self.structures[0] @property def final_structure(self): """The |Structure| of the last iteration.""" return self.structures[-1]
[docs] @lazy_property def structures(self): """List of |Structure| objects at the different steps.""" return self.reader.read_all_structures()
[docs] @lazy_property def etotals(self): """|numpy-array| with total energies in eV at the different steps.""" return self.reader.read_eterms().etotals
[docs] def get_relaxation_analyzer(self): """ Return a pymatgen :class:`RelaxationAnalyzer` object to analyze the relaxation in a calculation. """ return RelaxationAnalyzer(self.initial_structure, self.final_structure)
[docs] def to_xdatcar(self, filepath=None, groupby_type=True, to_unit_cell=False, **kwargs): """ Return Xdatcar pymatgen object. See write_xdatcar for the meaning of arguments. Args: to_unit_cell (bool): Whether to translate sites into the unit cell. kwargs: keywords arguments passed to Xdatcar constructor. """ filepath = self.write_xdatcar(filepath=filepath, groupby_type=groupby_type, to_unit_cell=to_unit_cell, overwrite=True) from pymatgen.io.vasp.outputs import Xdatcar return Xdatcar(filepath, **kwargs)
[docs] def write_xdatcar(self, filepath="XDATCAR", groupby_type=True, overwrite=False, to_unit_cell=False): """ Write Xdatcar file with unit cell and atomic positions to file ``filepath``. Args: filepath: Xdatcar filename. If None, a temporary file is created. groupby_type: If True, atoms are grouped by type. Note that this option may change the order of the atoms. This option is needed because there are post-processing tools (e.g. ovito) that do not work as expected if the atoms in the structure are not grouped by type. overwrite: raise RuntimeError, if False and filepath exists. to_unit_cell (bool): Whether to translate sites into the unit cell. Return: path to Xdatcar file. """ if filepath is not None and os.path.exists(filepath) and not overwrite: raise RuntimeError("Cannot overwrite pre-existing file `%s`" % filepath) if filepath is None: import tempfile fd, filepath = tempfile.mkstemp(text=True, suffix="_XDATCAR") # int typat[natom], double znucl[npsp] # NB: typat is double in the HIST.nc file typat = self.reader.read_value("typat").astype(int) znucl = self.reader.read_value("znucl") ntypat = self.reader.read_dimvalue("ntypat") num_pseudos = self.reader.read_dimvalue("npsp") if num_pseudos != ntypat: raise NotImplementedError("Alchemical mixing is not supported, num_pseudos != ntypat") #print("znucl:", znucl, "\ntypat:", typat) symb2pos = OrderedDict() symbols_atom = [] for iatom, itype in enumerate(typat): itype = itype - 1 symbol = Element.from_Z(int(znucl[itype])).symbol if symbol not in symb2pos: symb2pos[symbol] = [] symb2pos[symbol].append(iatom) symbols_atom.append(symbol) if not groupby_type: group_ids = np.arange(self.reader.natom) else: group_ids = [] for pos_list in symb2pos.values(): group_ids.extend(pos_list) group_ids = np.array(group_ids, dtype=int) comment = " %s\n" % self.initial_structure.formula with open(filepath, "wt") as fh: # comment line + scaling factor set to 1.0 fh.write(comment) fh.write("1.0\n") for vec in self.initial_structure.lattice.matrix: fh.write("%.12f %.12f %.12f\n" % (vec[0], vec[1], vec[2])) if not groupby_type: fh.write(" ".join(symbols_atom) + "\n") fh.write("1 " * len(symbols_atom) + "\n") else: fh.write(" ".join(symb2pos.keys()) + "\n") fh.write(" ".join(str(len(p)) for p in symb2pos.values()) + "\n") # Write atomic positions in reduced coordinates. xred_list = self.reader.read_value("xred") if to_unit_cell: xred_list = xred_list % 1 for step in range(self.num_steps): fh.write("Direct configuration= %d\n" % (step + 1)) frac_coords = xred_list[step, group_ids] for fs in frac_coords: fh.write("%.12f %.12f %.12f\n" % (fs[0], fs[1], fs[2])) return filepath
[docs] def visualize(self, appname="ovito", to_unit_cell=False): # pragma: no cover """ Visualize the crystalline structure with visualizer. See :class:`Visualizer` for the list of applications and formats supported. Args: to_unit_cell (bool): Whether to translate sites into the unit cell. """ if appname == "mayavi": return self.mayaview() # Get the Visualizer subclass from the string. from abipy.iotools import Visualizer visu = Visualizer.from_name(appname) if visu.name != "ovito": raise NotImplementedError("visualizer: %s" % visu.name) filepath = self.write_xdatcar(filepath=None, groupby_type=True, to_unit_cell=to_unit_cell) return visu(filepath)()
#if options.trajectories: # hist.mvplot_trajectories() #else: # hist.mvanimate()
[docs] def plot_ax(self, ax, what, fontsize=8, **kwargs): """ Helper function to plot quantity ``what`` on axis ``ax`` with matplotlib. Args: fontsize: fontsize for legend. kwargs are passed to matplotlib plot method. """ label = None if what == "energy": # Total energy in eV. marker = kwargs.pop("marker", "o") label = kwargs.pop("label", "Energy") ax.plot(self.steps, self.etotals, label=label, marker=marker, **kwargs) ax.set_ylabel('Energy (eV)') elif what == "abc": # Lattice parameters. mark = kwargs.pop("marker", None) markers = ["o", "^", "v"] if mark is None else 3 * [mark] for i, label in enumerate(["a", "b", "c"]): ax.plot(self.steps, [s.lattice.abc[i] for s in self.structures], label=label, marker=markers[i], **kwargs) ax.set_ylabel("abc (A)") elif what in ("a", "b", "c"): i = ("a", "b", "c").index(what) marker = kwargs.pop("marker", None) if marker is None: marker = {"a": "o", "b": "^", "c": "v"}[what] label = kwargs.pop("label", what) ax.plot(self.steps, [s.lattice.abc[i] for s in self.structures], label=label, marker=marker, **kwargs) ax.set_ylabel('%s (A)' % what) elif what == "angles": # Lattice Angles mark = kwargs.pop("marker", None) markers = ["o", "^", "v"] if mark is None else 3 * [mark] for i, label in enumerate(["alpha", "beta", "gamma"]): ax.plot(self.steps, [s.lattice.angles[i] for s in self.structures], label=label, marker=markers[i], **kwargs) ax.set_ylabel(r"$\alpha\beta\gamma$ (degree)") elif what in ("alpha", "beta", "gamma"): i = ("alpha", "beta", "gamma").index(what) marker = kwargs.pop("marker", None) if marker is None: marker = {"alpha": "o", "beta": "^", "gamma": "v"}[what] label = kwargs.pop("label", what) ax.plot(self.steps, [s.lattice.angles[i] for s in self.structures], label=label, marker=marker, **kwargs) ax.set_ylabel(r"$\%s$ (degree)" % what) elif what == "volume": marker = kwargs.pop("marker", "o") ax.plot(self.steps, [s.lattice.volume for s in self.structures], marker=marker, **kwargs) ax.set_ylabel(r'$V\, (A^3)$') elif what == "pressure": stress_cart_tensors, pressures = self.reader.read_cart_stress_tensors() marker = kwargs.pop("marker", "o") label = kwargs.pop("label", "P") ax.plot(self.steps, pressures, label=label, marker=marker, **kwargs) ax.set_ylabel('P (GPa)') elif what == "forces": forces_hist = self.reader.read_cart_forces() fmin_steps, fmax_steps, fmean_steps, fstd_steps = [], [], [], [] for step in range(self.num_steps): forces = forces_hist[step] fmods = np.sqrt([np.dot(force, force) for force in forces]) fmean_steps.append(fmods.mean()) fstd_steps.append(fmods.std()) fmin_steps.append(fmods.min()) fmax_steps.append(fmods.max()) mark = kwargs.pop("marker", None) markers = ["o", "^", "v", "X"] if mark is None else 4 * [mark] ax.plot(self.steps, fmin_steps, label="min |F|", marker=markers[0], **kwargs) ax.plot(self.steps, fmax_steps, label="max |F|", marker=markers[1], **kwargs) ax.plot(self.steps, fmean_steps, label="mean |F|", marker=markers[2], **kwargs) ax.plot(self.steps, fstd_steps, label="std |F|", marker=markers[3], **kwargs) label = "std |F|" ax.set_ylabel('F stats (eV/A)') else: raise ValueError("Invalid value for what: `%s`" % str(what)) ax.set_xlabel('Step') ax.grid(True) if label is not None: ax.legend(loc='best', fontsize=fontsize, shadow=True)
[docs] def plotly_traces(self, fig, what, rcd=None, fontsize=8, showlegend=False, **kwargs): """ Helper function to plot quantity ``what`` on figure ``fig`` with plotly. Args: rcd: If ``fig`` has subplots, ``rcd`` is used to add traces on these subplots. fontsize: fontsize for legend. kwargs are passed to fig.add_scatter method. """ rcd = PlotlyRowColDesc.from_object(rcd) ply_row, ply_col = rcd.ply_row, rcd.ply_col label = None if what == "energy": # Total energy in eV. marker = kwargs.pop("marker", 0) label = kwargs.pop("label", "Energy") fig.add_scatter(x=self.steps, y=self.etotals, mode='lines+markers', name=label, marker_symbol=marker, row=ply_row, col=ply_col, **kwargs) fig.layout['yaxis%u' % rcd.iax].title.text = 'Energy (eV)' elif what == "abc": # Lattice parameters. mark = kwargs.pop("marker", None) markers = [0, 5, 6] if mark is None else 3 * [mark] for i, label in enumerate(["a", "b", "c"]): fig.add_scatter(x=self.steps, y=[s.lattice.abc[i] for s in self.structures], mode='lines+markers', name=label, marker_symbol=markers[i], row=ply_row, col=ply_col, **kwargs) fig.layout['yaxis%u' % rcd.iax].title.text = "abc (A)" elif what in ("a", "b", "c"): i = ("a", "b", "c").index(what) marker = kwargs.pop("marker", None) if marker is None: marker = {"a": 0, "b": 5, "c": 6}[what] label = kwargs.pop("label", what) fig.add_scatter(x=self.steps, y=[s.lattice.abc[i] for s in self.structures], mode='lines+markers', name=label, marker_symbol=marker, row=ply_row, col=ply_col, **kwargs) fig.layout['yaxis%u' % rcd.iax].title.text = '%s (A)' % what elif what == "angles": # Lattice Angles mark = kwargs.pop("marker", None) markers = [0, 5, 6] if mark is None else 3 * [mark] for i, label in enumerate(["α ", "β ", "ɣ"]): fig.add_scatter(x=self.steps, y=[s.lattice.angles[i] for s in self.structures], mode='lines+markers', name=label, marker_symbol=markers[i], row=ply_row, col=ply_col, **kwargs) fig.layout['yaxis%u' % rcd.iax].title.text = "αβɣ (degree)"+ " " fig.layout['yaxis%u' % rcd.iax].tickformat = ".3r" elif what in ("alpha", "beta", "gamma"): i = ("alpha", "beta", "gamma").index(what) marker = kwargs.pop("marker", None) if marker is None: marker = {"alpha": 0, "beta": 5, "gamma": 6}[what] label = kwargs.pop("label", what) fig.add_scatter(x=self.steps, y=[s.lattice.angles[i] for s in self.structures], mode='lines+markers', name=label, marker_symbol=marker, row=ply_row, col=ply_col, **kwargs) fig.layout['yaxis%u' % rcd.iax].title.text = r"%s (degree)" % latex_greek_2unicode(what) fig.layout['yaxis%u' % rcd.iax].tickformat = ".3r" elif what == "volume": marker = kwargs.pop("marker", 0) label = kwargs.pop("label", "Volume") fig.add_scatter(x=self.steps, y=[s.lattice.volume for s in self.structures], mode='lines+markers', name=label, marker_symbol=marker, row=ply_row, col=ply_col, **kwargs) fig.layout['yaxis%u' % rcd.iax].title.text = 'V (A³)' elif what == "pressure": stress_cart_tensors, pressures = self.reader.read_cart_stress_tensors() marker = kwargs.pop("marker", 0) label = kwargs.pop("label", "P") fig.add_scatter(x=self.steps, y=pressures, mode='lines+markers', name=label, marker_symbol=marker, row=ply_row, col=ply_col, **kwargs) fig.layout['yaxis%u' % rcd.iax].title.text = 'P (GPa)' elif what == "forces": forces_hist = self.reader.read_cart_forces() fmin_steps, fmax_steps, fmean_steps, fstd_steps = [], [], [], [] for step in range(self.num_steps): forces = forces_hist[step] fmods = np.sqrt([np.dot(force, force) for force in forces]) fmean_steps.append(fmods.mean()) fstd_steps.append(fmods.std()) fmin_steps.append(fmods.min()) fmax_steps.append(fmods.max()) mark = kwargs.pop("marker", None) markers = [0, 5, 6, 4] if mark is None else 4 * [mark] fig.add_scatter(x=self.steps, y=fmin_steps, mode='lines+markers', name="min |F|", marker_symbol=markers[0], row=ply_row, col=ply_col, **kwargs) fig.add_scatter(x=self.steps, y=fmax_steps, mode='lines+markers', name="max |F|", marker_symbol=markers[1], row=ply_row, col=ply_col, **kwargs) fig.add_scatter(x=self.steps, y=fmean_steps, mode='lines+markers', name="mean |F|", marker_symbol=markers[2], row=ply_row, col=ply_col, **kwargs) fig.add_scatter(x=self.steps, y=fstd_steps, mode='lines+markers', name="std |F|", marker_symbol=markers[3], row=ply_row, col=ply_col, **kwargs) label = "std |F|" fig.layout['yaxis%u' % rcd.iax].title.text = 'F stats (eV/A)' else: raise ValueError("Invalid value for what: `%s`" % str(what)) fig.layout.legend.font.size = fontsize
[docs] @add_fig_kwargs def plot(self, what_list=None, ax_list=None, fontsize=8, **kwargs): """ Plot the evolution of structural parameters (lattice lengths, angles and volume) as well as pressure, info on forces and total energy with matplotlib. Args: what_list: ax_list: List of |matplotlib-Axes|. If None, a new figure is created. fontsize: fontsize for legend Returns: |matplotlib-Figure| """ if what_list is None: what_list = ["abc", "angles", "volume", "pressure", "forces", "energy"] else: what_list = list_strings(what_list) nplots = len(what_list) nrows, ncols = 1, 1 if nplots > 1: ncols = 2 nrows = nplots // ncols + nplots % ncols ax_list, fig, plt = get_axarray_fig_plt(ax_list, nrows=nrows, ncols=ncols, sharex=True, sharey=False, squeeze=False) ax_list = ax_list.ravel() # don't show the last ax if nplots is odd. if nplots % ncols != 0: ax_list[-1].axis("off") for what, ax in zip(what_list, ax_list): self.plot_ax(ax, what, fontsize=fontsize, marker="o") return fig
[docs] @add_plotly_fig_kwargs def plotly(self, what_list=None, fig=None, fontsize=12, **kwargs): """ Plot the evolution of structural parameters (lattice lengths, angles and volume) as well as pressure, info on forces and total energy with plotly. Args: what_list: fig: The fig for plot and the DOS plot. If None, a new figure is created. fontsize: fontsize for legend Returns: |plotly.graph_objects.Figure| """ if what_list is None: what_list = ["abc", "angles", "volume", "pressure", "forces", "energy"] else: what_list = list_strings(what_list) nplots = len(what_list) nrows, ncols = 1, 1 if nplots > 1: ncols = 2 nrows = nplots // ncols + nplots % ncols if fig is None: fig, _ = get_figs_plotly(nrows=nrows, ncols=ncols, subplot_titles=[], sharex=True, sharey=False, vertical_spacing=0.05) for i, what in enumerate(what_list): rcd = PlotlyRowColDesc(i // ncols, i % ncols, nrows, ncols) self.plotly_traces(fig, what, rcd=rcd, fontsize=fontsize, marker=0) fig.layout['xaxis%u' % rcd.iax].title.text = 'Step' if nplots > 1: fig.layout['xaxis%s' % str(rcd.iax-1)].title.text = 'Step' return fig
[docs] @add_fig_kwargs def plot_energies(self, ax=None, fontsize=8, **kwargs): """ Plot the total energies as function of the iteration step. Args: ax: |matplotlib-Axes| or None if a new figure should be created. fontsize: Legend and title fontsize. Returns: |matplotlib-Figure| """ # TODO max force and pressure ax, fig, plt = get_ax_fig_plt(ax=ax) terms = self.reader.read_eterms() for key, values in terms.items(): if np.all(values == 0.0): continue ax.plot(self.steps, values, marker="o", label=key) ax.set_xlabel('Step') ax.set_ylabel('Energies (eV)') ax.grid(True) ax.legend(loc='best', fontsize=fontsize, shadow=True) return fig
[docs] def yield_figs(self, **kwargs): # pragma: no cover """ This function *generates* a predefined list of matplotlib figures with minimal input from the user. """ yield self.plot(show=False) yield self.plot_energies(show=False)
[docs] def yield_plotly_figs(self, **kwargs): # pragma: no cover """ This function *generates* a predefined list of matplotlib figures with minimal input from the user. """ yield self.plotly(show=False)
#yield self.plotly_energies(show=False)
[docs] def mvplot_trajectories(self, colormap="hot", sampling=1, figure=None, show=True, with_forces=True, **kwargs): # pragma: no cover """ Call mayavi_ to plot atomic trajectories and the variation of the unit cell. """ from abipy.display import mvtk figure, mlab = mvtk.get_fig_mlab(figure=figure) style = "labels" line_width = 100 mvtk.plot_structure(self.initial_structure, style=style, unit_cell_color=(1, 0, 0), figure=figure) mvtk.plot_structure(self.final_structure, style=style, unit_cell_color=(0, 0, 0), figure=figure) steps = np.arange(start=0, stop=self.num_steps, step=sampling) xcart_list = self.reader.read_value("xcart") * units.bohr_to_ang for iatom in range(self.reader.natom): x, y, z = xcart_list[::sampling, iatom, :].T #for i in zip(x, y, z): print(i) trajectory = mlab.plot3d(x, y, z, steps, colormap=colormap, tube_radius=None, line_width=line_width, figure=figure) mlab.colorbar(trajectory, title='Iteration', orientation='vertical') if with_forces: fcart_list = self.reader.read_cart_forces(unit="eV ang^-1") for iatom in range(self.reader.natom): x, y, z = xcart_list[::sampling, iatom, :].T u, v, w = fcart_list[::sampling, iatom, :].T q = mlab.quiver3d(x, y, z, u, v, w, figure=figure, colormap=colormap, line_width=line_width, scale_factor=10) #mlab.colorbar(q, title='Forces [eV/Ang]', orientation='vertical') if show: mlab.show() return figure
[docs] def mvanimate(self, delay=500): # pragma: no cover from abipy.display import mvtk figure, mlab = mvtk.get_fig_mlab(figure=None) style = "points" #mvtk.plot_structure(self.initial_structure, style=style, figure=figure) #mvtk.plot_structure(self.final_structure, style=style, figure=figure) xcart_list = self.reader.read_value("xcart") * units.bohr_to_ang #t = np.arange(self.num_steps) #line_width = 2 #for iatom in range(self.reader.natom): # x, y, z = xcart_list[:, iatom, :].T # trajectory = mlab.plot3d(x, y, z, t, colormap=colormap, tube_radius=None, line_width=line_width, figure=figure) #mlab.colorbar(trajectory, title='Iteration', orientation='vertical') #x, y, z = xcart_list[0, :, :].T #nodes = mlab.points3d(x, y, z) #nodes.glyph.scale_mode = 'scale_by_vector' #this sets the vectors to be a 3x5000 vector showing some random scalars #nodes.mlab_source.dataset.point_data.vectors = np.tile( np.random.random((5000,)), (3,1)) #nodes.mlab_source.dataset.point_data.scalars = np.random.random((5000,)) @mlab.show @mlab.animate(delay=delay, ui=True) def anim(): """Animate.""" #for it in range(self.num_steps): for it, structure in enumerate(self.structures): print('Updating scene for iteration:', it) #mlab.clf(figure=figure) mvtk.plot_structure(structure, style=style, figure=figure) #x, y, z = xcart_list[it, :, :].T #nodes.mlab_source.set(x=x, y=y, z=z) #figure.scene.render() mlab.draw(figure=figure) yield anim()
[docs] def get_panel(self, **kwargs): """ Build panel with widgets to interact with the |HistFile| either in a notebook or in panel app. """ from abipy.panels.hist import HistFilePanel return HistFilePanel(self).get_panel(**kwargs)
[docs] def write_notebook(self, nbpath=None): """ Write a jupyter_ notebook to ``nbpath``. If nbpath is None, a temporay file in the current working directory is created. Return path to the notebook. """ nbformat, nbv, nb = self.get_nbformat_nbv_nb(title=None) nb.cells.extend([ #nbv.new_markdown_cell("# This is a markdown cell"), nbv.new_code_cell("hist = abilab.abiopen('%s')" % self.filepath), nbv.new_code_cell("print(hist)"), nbv.new_code_cell("hist.plot_energies();"), nbv.new_code_cell("hist.plot();"), ]) return self._write_nb_nbpath(nb, nbpath)
[docs]class HistRobot(Robot): """ This robot analyzes the results contained in multiple HIST.nc_ files. .. rubric:: Inheritance Diagram .. inheritance-diagram:: HistRobot """ EXT = "HIST"
[docs] def to_string(self, verbose=0): """String representation with verbosity level ``verbose``.""" s = "" if verbose: s = super().to_string(verbose=0) df = self.get_dataframe() s_df = "Table with final structures, pressures in GPa and force stats in eV/Ang:\n\n%s" % str(df) if s: return "\n".join([s, str(s_df)]) else: return str(s_df)
[docs] def get_dataframe(self, with_geo=True, index=None, abspath=False, with_spglib=True, funcs=None, **kwargs): """ Return a |pandas-DataFrame| with the most important final results and the filenames as index. Args: with_geo: True if structure info should be added to the dataframe abspath: True if paths in index should be absolute. Default: Relative to getcwd(). index: Index of the dataframe, if None, robot labels are used with_spglib: If True, spglib_ is invoked to get the space group symbol and number kwargs: attrs: List of additional attributes of the |GsrFile| to add to the |pandas-DataFrame|. funcs: Function or list of functions to execute to add more data to the DataFrame. Each function receives a |GsrFile| object and returns a tuple (key, value) where key is a string with the name of column and value is the value to be inserted. """ # Add attributes specified by the users attrs = [ "num_steps", "final_energy", "final_pressure", "final_fmin", "final_fmax", "final_fmean", "final_fstd", "final_drift", "initial_fmin", "initial_fmax", "initial_fmean", "initial_fstd", "initial_drift", # TODO add more columns but must update HIST file #"nsppol", "nspinor", "nspden", #"ecut", "pawecutdg", "tsmear", "nkpt", ] + kwargs.pop("attrs", []) rows, row_names = [], [] for label, hist in self.items(): row_names.append(label) d = OrderedDict() initial_fstas_dict = hist.get_fstats_dict(step=0) final_fstas_dict = hist.get_fstats_dict(step=-1) # Add info on structure. if with_geo: d.update(hist.final_structure.get_dict4pandas(with_spglib=with_spglib)) for aname in attrs: if aname in ("final_fmin", "final_fmax", "final_fmean", "final_fstd", "final_drift",): value = final_fstas_dict[aname.replace("final_", "")] elif aname in ("initial_fmin", "initial_fmax", "initial_fmean", "initial_fstd", "initial_drift"): value = initial_fstas_dict[aname.replace("initial_", "")] else: value = getattr(hist, aname, None) d[aname] = value # Execute functions if funcs is not None: d.update(self._exec_funcs(funcs, hist)) rows.append(d) import pandas as pd row_names = row_names if not abspath else self._to_relpaths(row_names) index = row_names if index is None else index return pd.DataFrame(rows, index=index, columns=list(rows[0].keys()))
@property def what_list(self): """List with all quantities that can be plotted (what_list).""" return ["energy", "abc", "angles", "volume", "pressure", "forces"]
[docs] @add_fig_kwargs def gridplot(self, what_list=None, sharex="row", sharey="row", fontsize=8, **kwargs): """ Plot the ``what`` value extracted from multiple HIST.nc_ files on a grid. Args: what_list: List of quantities to plot. Must be in ["energy", "abc", "angles", "volume", "pressure", "forces"] sharex: True if xaxis should be shared. sharey: True if yaxis should be shared. fontsize: fontsize for legend. Returns: |matplotlib-Figure| """ what_list = list_strings(what_list) if what_list is not None else self.what_list # Build grid of plots. nrows, ncols = len(what_list), len(self) ax_mat, fig, plt = get_axarray_fig_plt(None, nrows=nrows, ncols=ncols, sharex=sharex, sharey=sharey, squeeze=False) ax_mat = np.reshape(ax_mat, (nrows, ncols)) for irow, what in enumerate(what_list): for icol, hist in enumerate(self.abifiles): ax = ax_mat[irow, icol] ax.grid(True) hist.plot_ax(ax_mat[irow, icol], what, fontsize=fontsize, marker="o") if irow == 0: ax.set_title(hist.relpath, fontsize=fontsize) if irow != nrows - 1: set_visible(ax, False, "xlabel") if icol != 0: set_visible(ax, False, "ylabel") return fig
[docs] @add_fig_kwargs def combiplot(self, what_list=None, colormap="jet", fontsize=6, **kwargs): """ Plot multiple HIST.nc_ files on a grid. One plot for each ``what`` value. Args: what_list: List of strings with the quantities to plot. If None, all quanties are plotted. colormap: matplotlib color map. fontsize: fontisize for legend. Returns: |matplotlib-Figure|. """ what_list = (list_strings(what_list) if what_list is not None else ["energy", "a", "b", "c", "alpha", "beta", "gamma", "volume", "pressure"]) num_plots, ncols, nrows = len(what_list), 1, 1 if num_plots > 1: ncols = 2 nrows = (num_plots // ncols) + (num_plots % ncols) ax_list, fig, plt = get_axarray_fig_plt(None, nrows=nrows, ncols=ncols, sharex=True, sharey=False, squeeze=False) ax_list = ax_list.ravel() cmap = plt.get_cmap(colormap) for i, (ax, what) in enumerate(zip(ax_list, what_list)): for ih, hist in enumerate(self.abifiles): label = None if i != 0 else hist.relpath hist.plot_ax(ax, what, color=cmap(ih / len(self)), label=label, fontsize=fontsize) if label is not None: ax.legend(loc="best", fontsize=fontsize, shadow=True) if i == len(ax_list) - 1: ax.set_xlabel("Step") else: ax.set_xlabel("") # Get around a bug in matplotlib. if num_plots % ncols != 0: ax_list[-1].axis('off') return fig
[docs] def yield_figs(self, **kwargs): # pragma: no cover """ This function *generates* a predefined list of matplotlib figures with minimal input from the user. """ yield self.gridplot(show=False) yield self.combiplot(show=False)
[docs] def write_notebook(self, nbpath=None): """ Write a jupyter_ notebook to nbpath. If nbpath is None, a temporay file in the current working directory is created. Return path to the notebook. """ nbformat, nbv, nb = self.get_nbformat_nbv_nb(title=None) args = [(l, f.filepath) for l, f in self.items()] nb.cells.extend([ #nbv.new_markdown_cell("# This is a markdown cell"), nbv.new_code_cell("robot = abilab.HistRobot(*%s)\nrobot.trim_paths()\nrobot" % str(args)), nbv.new_code_cell("robot.get_dataframe()"), nbv.new_code_cell("for what in robot.what_list: robot.gridplot(what=what, tight_layout=True);"), ]) # Mixins #nb.cells.extend(self.get_baserobot_code_cells()) return self._write_nb_nbpath(nb, nbpath)
[docs]class HistReader(ETSF_Reader): """ This object reads data from the HIST file. .. rubric:: Inheritance Diagram .. inheritance-diagram:: HistReader """
[docs] @lazy_property def num_steps(self): """Number of iterations present in the HIST.nc_ file.""" return self.read_dimvalue("time")
[docs] @lazy_property def natom(self): """Number of atoms un the unit cell.""" return self.read_dimvalue("natom")
[docs] def read_all_structures(self): """Return the list of structures at the different iteration steps.""" rprimd_list = self.read_value("rprimd") xred_list = self.read_value("xred") # Alchemical mixing is not supported. num_pseudos = self.read_dimvalue("npsp") ntypat = self.read_dimvalue("ntypat") if num_pseudos != ntypat: raise NotImplementedError("Alchemical mixing is not supported, num_pseudos != ntypat") znucl, typat = self.read_value("znucl"), self.read_value("typat").astype(int) #print(znucl.dtype, typat) cart_forces_step = self.read_cart_forces(unit="eV ang^-1") structures = [] #print("typat", type(typat)) for step in range(self.num_steps): s = Structure.from_abivars( xred=xred_list[step], rprim=rprimd_list[step], acell=3 * [1.0], # FIXME ntypat, typat, znucl are missing! znucl=znucl, typat=typat, ) s.add_site_property("cartesian_forces", cart_forces_step[step]) structures.append(s) return structures
[docs] def read_eterms(self, unit="eV"): """|AttrDict| with the decomposition of the total energy in units ``unit``""" return AttrDict( etotals=units.EnergyArray(self.read_value("etotal"), "Ha").to(unit), kinetic_terms=units.EnergyArray(self.read_value("ekin"), "Ha").to(unit), entropies=units.EnergyArray(self.read_value("entropy"), "Ha").to(unit), )
[docs] def read_cart_forces(self, unit="eV ang^-1"): """ Read and return a |numpy-array| with the cartesian forces in unit ``unit``. Shape (num_steps, natom, 3) """ return units.ArrayWithUnit(self.read_value("fcart"), "Ha bohr^-1").to(unit)
[docs] def read_reduced_forces(self): """ Read and return a |numpy-array| with the forces in reduced coordinates Shape (num_steps, natom, 3) """ return self.read_value("fred")
[docs] def read_cart_stress_tensors(self): """ Return the stress tensors (nstep x 3 x 3) in cartesian coordinates (GPa) and the list of pressures in GPa unit. """ # Abinit stores 6 unique components of this symmetric 3x3 tensor: # Given in order (1,1), (2,2), (3,3), (3,2), (3,1), (2,1). c = self.read_value("strten") tensors = np.empty((self.num_steps, 3, 3), dtype=float) for step in range(self.num_steps): for i in range(3): tensors[step, i,i] = c[step, i] for p, (i, j) in enumerate(((2,1), (2,0), (1,0))): tensors[step, i,j] = c[step, 3+p] tensors[step, j,i] = c[step, 3+p] tensors *= abu.HaBohr3_GPa pressures = np.empty(self.num_steps) for step, tensor in enumerate(tensors): pressures[step] = - tensor.trace() / 3 return tensors, pressures