# Source code for pymatgen.analysis.diffusion_analyzer

    # coding: utf-8
    # Copyright (c) Pymatgen Development Team.
    # Distributed under the terms of the MIT License.

    """
    A module to perform diffusion analyses (e.g. calculating diffusivity from
    mean square displacements etc.). If you use this module, please consider
    citing the following papers::

        Ong, S. P., Mo, Y., Richards, W. D., Miara, L., Lee, H. S., & Ceder, G.
        (2013). Phase stability, electrochemical stability and ionic conductivity
        of the Li10+-1MP2X12 (M = Ge, Si, Sn, Al or P, and X = O, S or Se) family
        of superionic conductors. Energy & Environmental Science, 6(1), 148.
        doi:10.1039/c2ee23355j

        Mo, Y., Ong, S. P., & Ceder, G. (2012). First Principles Study of the
        Li10GeP2S12 Lithium Super Ionic Conductor Material. Chemistry of Materials,
        24(1), 15-17. doi:10.1021/cm203303y
    """

    import numpy as np
    import warnings
    import scipy.constants as const

    from monty.json import MSONable

    from pymatgen.analysis.structure_matcher import StructureMatcher, \
        OrderDisorderElementComparator
    from pymatgen.core.periodic_table import get_el_sp
    from pymatgen.core.structure import Structure
    from pymatgen.io.vasp.outputs import Vasprun
    from pymatgen.util.coord import pbc_diff

    __author__ = "Will Richards, Shyue Ping Ong"
    __version__ = "0.2"
    __maintainer__ = "Will Richards"
    __email__ = "wrichard@mit.edu"
    __status__ = "Beta"
    __date__ = "5/2/13"

    class DiffusionAnalyzer(MSONable):
        """
        Class for performing diffusion analysis.

        .. attribute: diffusivity

            Diffusivity in cm^2 / s

        .. attribute: chg_diffusivity

            Charge diffusivity in cm^2 / s

        .. attribute: conductivity

            Conductivity in mS / cm

        .. attribute: chg_conductivity

            Conductivity derived from Nernst-Einstein equation using charge
            diffusivity, in mS / cm

        .. attribute: diffusivity_components

            A vector with diffusivity in the a, b and c directions in cm^2 / s

        .. attribute: conductivity_components

            A vector with conductivity in the a, b and c directions in mS / cm

        .. attribute: diffusivity_std_dev

            Std dev in diffusivity in cm^2 / s. Note that this makes sense only
            for non-smoothed analyses.

        .. attribute: chg_diffusivity_std_dev

            Std dev in charge diffusivity in cm^2 / s. Note that this makes sense only
            for non-smoothed analyses.

        .. attribute: conductivity_std_dev

            Std dev in conductivity in mS / cm. Note that this makes sense only
            for non-smoothed analyses.

        .. attribute: diffusivity_components_std_dev

            A vector with std dev. in diffusivity in the a, b and c directions in
            cm^2 / cm. Note that this makes sense only for non-smoothed analyses.

        .. attribute: conductivity_components_std_dev

            A vector with std dev. in conductivity in the a, b and c directions
            in mS / cm. Note that this makes sense only for non-smoothed analyses.

        .. attribute: max_framework_displacement

            The maximum (drift adjusted) distance of any framework atom from its
            starting location in A.

        .. attribute: max_ion_displacements

            nions x 1 array of the maximum displacement of each individual ion.

        .. attribute: msd

            nsteps x 1 array of the mean square displacement of specie.

        .. attribute: mscd

            nsteps x 1 array of the mean square charge displacement of specie.

        .. attribute: msd_components

            nsteps x 3 array of the MSD in each lattice direction of specie.

        .. attribute: sq_disp_ions

            The square displacement of all ion (both specie and other ions) as a
            nions x nsteps array.

        .. attribute: dt

            Time coordinate array.

        .. attribute: haven_ratio
            Haven ratio defined as diffusivity / chg_diffusivity.
        """

        def __init__(self, structure, displacements, specie, temperature,
                     time_step, step_skip, smoothed="max", min_obs=30,
                     avg_nsteps=1000, lattices=None):
            """
            This constructor is meant to be used with pre-processed data.
            Other convenient constructors are provided as class methods (see
            from_vaspruns and from_files).

            Given a matrix of displacements (see arguments below for expected
            format), the diffusivity is given by::

                D = 1 / 2dt * <mean square displacement>

            where d is the dimensionality, t is the time. To obtain a reliable
            diffusion estimate, a least squares regression of the MSD against
            time to obtain the slope, which is then related to the diffusivity.

            For traditional analysis, use smoothed=False and weighted=False.

            Args:
                structure (Structure): Initial structure.
                displacements (array): Numpy array of with shape [site,
                    time step, axis]
                specie (Element/Specie): Specie to calculate diffusivity for as a
                    String. E.g., "Li".
                temperature (float): Temperature of the diffusion run in Kelvin.
                time_step (int): Time step between measurements.
                step_skip (int): Sampling frequency of the displacements (
                    time_step is multiplied by this number to get the real time
                    between measurements)
                smoothed (str): Whether to smooth the MSD, and what mode to smooth.
                    Supported modes are:

                    i. "max", which tries to use the maximum #
                       of data points for each time origin, subject to a
                       minimum # of observations given by min_obs, and then
                       weights the observations based on the variance
                       accordingly. This is the default.
                    ii. "constant", in which each timestep is averaged over
                        the number of time_steps given by min_steps.
                    iii. None / False / any other false-like quantity. No
                       smoothing.

                min_obs (int): Used with smoothed="max". Minimum number of
                    observations to have before including in the MSD vs dt
                    calculation. E.g. If a structure has 10 diffusing atoms,
                    and min_obs = 30, the MSD vs dt will be
                    calculated up to dt = total_run_time / 3, so that each
                    diffusing atom is measured at least 3 uncorrelated times.
                    Only applies in smoothed="max".
                avg_nsteps (int): Used with smoothed="constant". Determines the
                    number of time steps to average over to get the msd for each
                    timestep. Default of 1000 is usually pretty good.
                lattices (array): Numpy array of lattice matrix of every step. Used
                    for NPT-AIMD. For NVT-AIMD, the lattice at each time step is
                    set to the lattice in the "structure" argument.
            """
            self.structure = structure
            self.disp = displacements
            self.specie = specie
            self.temperature = temperature
            self.time_step = time_step
            self.step_skip = step_skip
            self.min_obs = min_obs
            self.smoothed = smoothed
            self.avg_nsteps = avg_nsteps
            self.lattices = lattices

            if lattices is None:
                self.lattices = np.array([structure.lattice.matrix.tolist()])

            indices = []
            framework_indices = []
            for i, site in enumerate(structure):
                if site.specie.symbol == specie:
                    indices.append(i)
                else:
                    framework_indices.append(i)
            if self.disp.shape[1] < 2:
                self.diffusivity = 0.
                self.conductivity = 0.
                self.diffusivity_components = np.array([0., 0., 0.])
                self.conductivity_components = np.array([0., 0., 0.])
                self.max_framework_displacement = 0
            else:
                framework_disp = self.disp[framework_indices]
                drift = np.average(framework_disp, axis=0)[None, :, :]

                # drift corrected position
                dc = self.disp - drift

                nions, nsteps, dim = dc.shape

                if not smoothed:
                    timesteps = np.arange(0, nsteps)
                elif smoothed == "constant":
                    if nsteps <= avg_nsteps:
                        raise ValueError('Not enough data to calculate diffusivity')
                    timesteps = np.arange(0, nsteps - avg_nsteps)
                else:
                    # limit the number of sampled timesteps to 200
                    min_dt = int(1000 / (self.step_skip * self.time_step))
                    max_dt = min(len(indices) * nsteps // self.min_obs, nsteps)
                    if min_dt >= max_dt:
                        raise ValueError('Not enough data to calculate diffusivity')
                    timesteps = np.arange(min_dt, max_dt,
                                          max(int((max_dt - min_dt) / 200), 1))

                dt = timesteps * self.time_step * self.step_skip

                # calculate the smoothed msd values
                msd = np.zeros_like(dt, dtype=np.double)
                sq_disp_ions = np.zeros((len(dc), len(dt)), dtype=np.double)
                msd_components = np.zeros(dt.shape + (3,))

                # calculate mean square charge displacement
                mscd = np.zeros_like(msd, dtype=np.double)

                for i, n in enumerate(timesteps):
                    if not smoothed:
                        dx = dc[:, i:i + 1, :]
                        dcomponents = dc[:, i:i + 1, :]
                    elif smoothed == "constant":
                        dx = dc[:, i:i + avg_nsteps, :] - dc[:, 0:avg_nsteps, :]
                        dcomponents = dc[:, i:i + avg_nsteps, :] - dc[:, 0:avg_nsteps, :]
                    else:
                        dx = dc[:, n:, :] - dc[:, :-n, :]
                        dcomponents = dc[:, n:, :] - dc[:, :-n, :]

                    # Get msd
                    sq_disp = dx ** 2
                    sq_disp_ions[:, i] = np.average(np.sum(sq_disp, axis=2), axis=1)
                    msd[i] = np.average(sq_disp_ions[:, i][indices])

                    msd_components[i] = np.average(dcomponents[indices] ** 2,
                                                   axis=(0, 1))

                    # Get mscd
                    sq_chg_disp = np.sum(dx[indices, :, :], axis=0) ** 2
                    mscd[i] = np.average(np.sum(sq_chg_disp, axis=1), axis=0) / len(indices)

                def weighted_lstsq(a, b):
                    if smoothed == "max":
                        # For max smoothing, we need to weight by variance.
                        w_root = (1 / dt) ** 0.5
                        return np.linalg.lstsq(
                            a * w_root[:, None], b * w_root, rcond=None)
                    else:
                        return np.linalg.lstsq(a, b, rcond=None)

                # Get self diffusivity
                m_components = np.zeros(3)
                m_components_res = np.zeros(3)
                a = np.ones((len(dt), 2))
                a[:, 0] = dt
                for i in range(3):
                    (m, c), res, rank, s = weighted_lstsq(a, msd_components[:, i])
                    m_components[i] = max(m, 1e-15)
                    m_components_res[i] = res[0]

                (m, c), res, rank, s = weighted_lstsq(a, msd)
                # m shouldn't be negative
                m = max(m, 1e-15)

                # Get also the charge diffusivity
                (m_chg, c_chg), res_chg, _, _ = weighted_lstsq(a, mscd)
                # m shouldn't be negative
                m_chg = max(m_chg, 1e-15)

                # factor of 10 is to convert from A^2/fs to cm^2/s
                # factor of 6 is for dimensionality
                conv_factor = get_conversion_factor(self.structure, self.specie,
                                                    self.temperature)
                self.diffusivity = m / 60
                self.chg_diffusivity = m_chg / 60

                # Calculate the error in the diffusivity using the error in the
                # slope from the lst sq.
                # Variance in slope = n * Sum Squared Residuals / (n * Sxx - Sx
                # ** 2) / (n-2).
                n = len(dt)

                # Pre-compute the denominator since we will use it later.
                # We divide dt by 1000 to avoid overflow errors in some systems (
                # e.g., win). This is subsequently corrected where denom is used.
                denom = (n * np.sum((dt / 1000) ** 2) - np.sum(dt / 1000) ** 2) * (
                        n - 2)
                self.diffusivity_std_dev = np.sqrt(n * res[0] / denom) / 60 / 1000
                self.chg_diffusivity_std_dev = np.sqrt(n * res_chg[0] / denom) / 60 / 1000
                self.conductivity = self.diffusivity * conv_factor
                self.chg_conductivity = self.chg_diffusivity * conv_factor
                self.conductivity_std_dev = self.diffusivity_std_dev * conv_factor

                self.diffusivity_components = m_components / 20
                self.diffusivity_components_std_dev = np.sqrt(
                    n * m_components_res / denom) / 20 / 1000
                self.conductivity_components = self.diffusivity_components * conv_factor
                self.conductivity_components_std_dev = self.diffusivity_components_std_dev * conv_factor

                # Drift and displacement information.
                self.drift = drift
                self.corrected_displacements = dc
                self.max_ion_displacements = np.max(np.sum(
                    dc ** 2, axis=-1) ** 0.5, axis=1)
                self.max_framework_displacement = \
                    np.max(self.max_ion_displacements[framework_indices])
                self.msd = msd
                self.mscd = mscd
                self.haven_ratio = self.diffusivity / self.chg_diffusivity
                self.sq_disp_ions = sq_disp_ions
                self.msd_components = msd_components
                self.dt = dt
                self.indices = indices
                self.framework_indices = framework_indices

        def get_drift_corrected_structures(self, start=None, stop=None, step=None):
            """
            Returns an iterator for the drift-corrected structures. Use of
            iterator is to reduce memory usage as # of structures in MD can be
            huge. You don't often need all the structures all at once.

            Args:
                start, stop, step (int): applies a start/stop/step to the iterator.
                    Faster than applying it after generation, as it reduces the
                    number of structures created.
            """
            coords = np.array(self.structure.cart_coords)
            species = self.structure.species_and_occu
            lattices = self.lattices
            nsites, nsteps, dim = self.corrected_displacements.shape

            for i in range(start or 0, stop or nsteps, step or 1):
                latt = lattices[0] if len(lattices) == 1 else lattices[i]
                yield Structure(
                    latt, species,
                    coords + self.corrected_displacements[:, i, :],
                    coords_are_cartesian=True)

        def get_summary_dict(self, include_msd_t=False, include_mscd_t=False):
            """
            Provides a summary of diffusion information.

            Args:
                include_msd_t (bool): Whether to include mean square displace and
                    time data with the data.
                include_msd_t (bool): Whether to include mean square charge displace and
                    time data with the data.

            Returns:
                (dict) of diffusion and conductivity data.
            """
            d = {
                "D": self.diffusivity,
                "D_sigma": self.diffusivity_std_dev,
                "D_charge": self.chg_diffusivity,
                "D_charge_sigma": self.chg_diffusivity_std_dev,
                "S": self.conductivity,
                "S_sigma": self.conductivity_std_dev,
                "S_charge": self.chg_conductivity,
                "D_components": self.diffusivity_components.tolist(),
                "S_components": self.conductivity_components.tolist(),
                "D_components_sigma": self.diffusivity_components_std_dev.tolist(),
                "S_components_sigma": self.conductivity_components_std_dev.tolist(),
                "specie": str(self.specie),
                "step_skip": self.step_skip,
                "time_step": self.time_step,
                "temperature": self.temperature,
                "max_framework_displacement": self.max_framework_displacement,
                "Haven_ratio": self.haven_ratio
            }
            if include_msd_t:
                d["msd"] = self.msd.tolist()
                d["msd_components"] = self.msd_components.tolist()
                d["dt"] = self.dt.tolist()
            if include_mscd_t:
                d["mscd"] = self.mscd.tolist()
            return d

        def get_framework_rms_plot(self, plt=None, granularity=200,
                                   matching_s=None):
            """
            Get the plot of rms framework displacement vs time. Useful for checking
            for melting, especially if framework atoms can move via paddle-wheel
            or similar mechanism (which would show up in max framework displacement
            but doesn't constitute melting).

            Args:
                plt (matplotlib.pyplot): If plt is supplied, changes will be made
                    to an existing plot. Otherwise, a new plot will be created.
                granularity (int): Number of structures to match
                matching_s (Structure): Optionally match to a disordered structure
                    instead of the first structure in the analyzer. Required when
                    a secondary mobile ion is present.
            Notes:
                The method doesn't apply to NPT-AIMD simulation analysis.
            """
            from pymatgen.util.plotting import pretty_plot
            if self.lattices is not None and len(self.lattices) > 1:
                warnings.warn("Note the method doesn't apply to NPT-AIMD "
                              "simulation analysis!")

            plt = pretty_plot(12, 8, plt=plt)
            step = (self.corrected_displacements.shape[1] - 1) // (granularity - 1)
            f = (matching_s or self.structure).copy()
            f.remove_species([self.specie])
            sm = StructureMatcher(primitive_cell=False, stol=0.6,
                                  comparator=OrderDisorderElementComparator(),
                                  allow_subset=True)
            rms = []
            for s in self.get_drift_corrected_structures(step=step):
                s.remove_species([self.specie])
                d = sm.get_rms_dist(f, s)
                if d:
                    rms.append(d)
                else:
                    rms.append((1, 1))
            max_dt = (len(rms) - 1) * step * self.step_skip * self.time_step
            if max_dt > 100000:
                plot_dt = np.linspace(0, max_dt / 1000, len(rms))
                unit = 'ps'
            else:
                plot_dt = np.linspace(0, max_dt, len(rms))
                unit = 'fs'
            rms = np.array(rms)
            plt.plot(plot_dt, rms[:, 0], label='RMS')
            plt.plot(plot_dt, rms[:, 1], label='max')
            plt.legend(loc='best')
            plt.xlabel("Timestep ({})".format(unit))
            plt.ylabel("normalized distance")
            plt.tight_layout()
            return plt

        def get_msd_plot(self, plt=None, mode="specie"):
            """
            Get the plot of the smoothed msd vs time graph. Useful for
            checking convergence. This can be written to an image file.

            Args:
                plt: A plot object. Defaults to None, which means one will be
                    generated.
                mode (str): Determines type of msd plot. By "species", "sites",
                    or direction (default). If mode = "mscd", the smoothed mscd vs.
                    time will be plotted.
            """
            from pymatgen.util.plotting import pretty_plot
            plt = pretty_plot(12, 8, plt=plt)
            if np.max(self.dt) > 100000:
                plot_dt = self.dt / 1000
                unit = 'ps'
            else:
                plot_dt = self.dt
                unit = 'fs'

            if mode == "species":
                for sp in sorted(self.structure.composition.keys()):
                    indices = [i for i, site in enumerate(self.structure) if
                               site.specie == sp]
                    sd = np.average(self.sq_disp_ions[indices, :], axis=0)
                    plt.plot(plot_dt, sd, label=sp.__str__())
                plt.legend(loc=2, prop={"size": 20})
            elif mode == "sites":
                for i, site in enumerate(self.structure):
                    sd = self.sq_disp_ions[i, :]
                    plt.plot(plot_dt, sd, label="%s - %d" % (
                        site.specie.__str__(), i))
                plt.legend(loc=2, prop={"size": 20})
            elif mode == "mscd":
                plt.plot(plot_dt, self.mscd, 'r')
                plt.legend(["Overall"], loc=2, prop={"size": 20})
            else:
                # Handle default / invalid mode case
                plt.plot(plot_dt, self.msd, 'k')
                plt.plot(plot_dt, self.msd_components[:, 0], 'r')
                plt.plot(plot_dt, self.msd_components[:, 1], 'g')
                plt.plot(plot_dt, self.msd_components[:, 2], 'b')
                plt.legend(["Overall", "a", "b", "c"], loc=2, prop={"size": 20})

            plt.xlabel("Timestep ({})".format(unit))
            if mode == "mscd":
                plt.ylabel("MSCD ($\\AA^2$)")
            else:
                plt.ylabel("MSD ($\\AA^2$)")
            plt.tight_layout()
            return plt

        def plot_msd(self, mode="default"):
            """
            Plot the smoothed msd vs time graph. Useful for checking convergence.

            Args:
                mode (str): Can be "default" (the default, shows only the MSD for
                    the diffusing specie, and its components), "ions" (individual
                    square displacements of all ions), "species" (mean square
                    displacement by specie), or "mscd" (overall mean square charge
                    displacement for diffusing specie).
            """
            self.get_msd_plot(mode=mode).show()

        def export_msdt(self, filename):
            """
            Writes MSD data to a csv file that can be easily plotted in other
            software.

            Args:
                filename (str): Filename. Supported formats are csv and dat. If
                    the extension is csv, a csv file is written. Otherwise,
                    a dat format is assumed.
            """
            fmt = "csv" if filename.lower().endswith(".csv") else "dat"
            delimiter = ", " if fmt == "csv" else " "
            with open(filename, "wt") as f:
                if fmt == "dat":
                    f.write("# ")
                f.write(delimiter.join(["t", "MSD", "MSD_a", "MSD_b", "MSD_c",
                                        "MSCD"]))
                f.write("\n")
                for dt, msd, msdc, mscd in zip(self.dt, self.msd,
                                               self.msd_components, self.mscd):
                    f.write(delimiter.join(["%s" % v for v in [dt, msd] + list(
                        msdc) + [mscd]]))
                    f.write("\n")

        @classmethod
        def from_structures(cls, structures, specie, temperature,
                            time_step, step_skip, initial_disp=None,
                            initial_structure=None, **kwargs):
            r"""
            Convenient constructor that takes in a list of Structure objects to
            perform diffusion analysis.

            Args:
                structures ([Structure]): list of Structure objects (must be
                    ordered in sequence of run). E.g., you may have performed
                    sequential VASP runs to obtain sufficient statistics.
                specie (Element/Specie): Specie to calculate diffusivity for as a
                    String. E.g., "Li".
                temperature (float): Temperature of the diffusion run in Kelvin.
                time_step (int): Time step between measurements.
                step_skip (int): Sampling frequency of the displacements (
                    time_step is multiplied by this number to get the real time
                    between measurements)
                initial_disp (np.ndarray): Sometimes, you need to iteratively
                    compute estimates of the diffusivity. This supplies an
                    initial displacement that will be added on to the initial
                    displacements. Note that this makes sense only when
                    smoothed=False.
                initial_structure (Structure): Like initial_disp, this is used
                    for iterative computations of estimates of the diffusivity. You
                    typically need to supply both variables. This stipulates the
                    initial structure from which the current set of displacements
                    are computed.
                \\*\\*kwargs: kwargs supported by the :class:`DiffusionAnalyzer`_.
                    Examples include smoothed, min_obs, avg_nsteps.
            """
            p, l = [], []
            for i, s in enumerate(structures):
                if i == 0:
                    structure = s
                p.append(np.array(s.frac_coords)[:, None])
                l.append(s.lattice.matrix)
            if initial_structure is not None:
                p.insert(0, np.array(initial_structure.frac_coords)[:, None])
                l.insert(0, initial_structure.lattice.matrix)
            else:
                p.insert(0, p[0])
                l.insert(0, l[0])

            p = np.concatenate(p, axis=1)
            dp = p[:, 1:] - p[:, :-1]
            dp = dp - np.round(dp)
            f_disp = np.cumsum(dp, axis=1)
            c_disp = []
            for i in f_disp:
                c_disp.append([np.dot(d, m) for d, m in zip(i, l[1:])])
            disp = np.array(c_disp)

            # If is NVT-AIMD, clear lattice data.
            if np.array_equal(l[0], l[-1]):
                l = np.array([l[0]])
            else:
                l = np.array(l)
            if initial_disp is not None:
                disp += initial_disp[:, None, :]

            return cls(structure, disp, specie, temperature, time_step,
                       step_skip=step_skip, lattices=l, **kwargs)

        @classmethod
        def from_vaspruns(cls, vaspruns, specie, initial_disp=None,
                          initial_structure=None, **kwargs):
            r"""
            Convenient constructor that takes in a list of Vasprun objects to
            perform diffusion analysis.

            Args:
                vaspruns ([Vasprun]): List of Vaspruns (must be ordered  in
                    sequence of MD simulation). E.g., you may have performed
                    sequential VASP runs to obtain sufficient statistics.
                specie (Element/Specie): Specie to calculate diffusivity for as a
                    String. E.g., "Li".
                initial_disp (np.ndarray): Sometimes, you need to iteratively
                    compute estimates of the diffusivity. This supplies an
                    initial displacement that will be added on to the initial
                    displacements. Note that this makes sense only when
                    smoothed=False.
                initial_structure (Structure): Like initial_disp, this is used
                    for iterative computations of estimates of the diffusivity. You
                    typically need to supply both variables. This stipulates the
                    initial stricture from which the current set of displacements
                    are computed.
                \\*\\*kwargs: kwargs supported by the :class:`DiffusionAnalyzer`_.
                    Examples include smoothed, min_obs, avg_nsteps.
            """

            def get_structures(vaspruns):
                for i, vr in enumerate(vaspruns):
                    if i == 0:
                        step_skip = vr.ionic_step_skip or 1
                        final_structure = vr.initial_structure
                        temperature = vr.parameters['TEEND']
                        time_step = vr.parameters['POTIM']
                        yield step_skip, temperature, time_step
                    # check that the runs are continuous
                    fdist = pbc_diff(vr.initial_structure.frac_coords,
                                     final_structure.frac_coords)
                    if np.any(fdist > 0.001):
                        raise ValueError('initial and final structures do not '
                                         'match.')
                    final_structure = vr.final_structure

                    assert (vr.ionic_step_skip or 1) == step_skip
                    for s in vr.ionic_steps:
                        yield s['structure']

            s = get_structures(vaspruns)
            step_skip, temperature, time_step = next(s)

            return cls.from_structures(
                structures=list(s), specie=specie, temperature=temperature,
                time_step=time_step, step_skip=step_skip,
                initial_disp=initial_disp, initial_structure=initial_structure,
                **kwargs)

        @classmethod
        def from_files(cls, filepaths, specie, step_skip=10, ncores=None,
                       initial_disp=None, initial_structure=None, **kwargs):
            r"""
            Convenient constructor that takes in a list of vasprun.xml paths to
            perform diffusion analysis.

            Args:
                filepaths ([str]): List of paths to vasprun.xml files of runs. (
                    must be ordered in sequence of MD simulation). For example,
                    you may have done sequential VASP runs and they are in run1,
                    run2, run3, etc. You should then pass in
                    ["run1/vasprun.xml", "run2/vasprun.xml", ...].
                specie (Element/Specie): Specie to calculate diffusivity for as a
                    String. E.g., "Li".
                step_skip (int): Sampling frequency of the displacements (
                    time_step is multiplied by this number to get the real time
                    between measurements)
                ncores (int): Numbers of cores to use for multiprocessing. Can
                    speed up vasprun parsing considerably. Defaults to None,
                    which means serial. It should be noted that if you want to
                    use multiprocessing, the number of ionic steps in all vasprun
                    .xml files should be a multiple of the ionic_step_skip.
                    Otherwise, inconsistent results may arise. Serial mode has no
                    such restrictions.
                initial_disp (np.ndarray): Sometimes, you need to iteratively
                    compute estimates of the diffusivity. This supplies an
                    initial displacement that will be added on to the initial
                    displacements. Note that this makes sense only when
                    smoothed=False.
                initial_structure (Structure): Like initial_disp, this is used
                    for iterative computations of estimates of the diffusivity. You
                    typically need to supply both variables. This stipulates the
                    initial structure from which the current set of displacements
                    are computed.
                \\*\\*kwargs: kwargs supported by the :class:`DiffusionAnalyzer`_.
                    Examples include smoothed, min_obs, avg_nsteps.
            """
            if ncores is not None and len(filepaths) > 1:
                import multiprocessing
                p = multiprocessing.Pool(ncores)
                vaspruns = p.imap(_get_vasprun,
                                  [(fp, step_skip) for fp in filepaths])
                analyzer = cls.from_vaspruns(
                    vaspruns, specie=specie, initial_disp=initial_disp,
                    initial_structure=initial_structure, **kwargs)
                p.close()
                p.join()
                return analyzer
            else:
                def vr(filepaths):
                    offset = 0
                    for p in filepaths:
                        v = Vasprun(p, ionic_step_offset=offset,
                                    ionic_step_skip=step_skip)
                        yield v
                        # Recompute offset.
                        offset = (-(v.nionic_steps - offset)) % step_skip

                return cls.from_vaspruns(
                    vr(filepaths), specie=specie, initial_disp=initial_disp,
                    initial_structure=initial_structure, **kwargs)

        def as_dict(self):
            """
            Returns: MSONable dict
            """
            return {
                "@module": self.__class__.__module__,
                "@class": self.__class__.__name__,
                "structure": self.structure.as_dict(),
                "displacements": self.disp.tolist(),
                "specie": self.specie,
                "temperature": self.temperature,
                "time_step": self.time_step,
                "step_skip": self.step_skip,
                "min_obs": self.min_obs,
                "smoothed": self.smoothed,
                "avg_nsteps": self.avg_nsteps,
                "lattices": self.lattices.tolist()
            }

        @classmethod
        def from_dict(cls, d):
            """
            Args:
                d (dict): Dict representation

            Returns: DiffusionAnalyzer
            """
            structure = Structure.from_dict(d["structure"])
            return cls(structure, np.array(d["displacements"]), specie=d["specie"],
                       temperature=d["temperature"], time_step=d["time_step"],
                       step_skip=d["step_skip"], min_obs=d["min_obs"],
                       smoothed=d.get("smoothed", "max"),
                       avg_nsteps=d.get("avg_nsteps", 1000),
                       lattices=np.array(d.get("lattices",
                                               [d["structure"]["lattice"][
                                                    "matrix"]])))

    def get_conversion_factor(structure, species, temperature):
        """
        Conversion factor to convert between cm^2/s diffusivity measurements and
        mS/cm conductivity measurements based on number of atoms of diffusing
        species. Note that the charge is based on the oxidation state of the
        species (where available), or else the number of valence electrons
        (usually a good guess, esp for main group ions).

        Args:
            structure (Structure): Input structure.
            species (Element/Specie): Diffusing species.
            temperature (float): Temperature of the diffusion run in Kelvin.

        Returns:
            Conversion factor.
            Conductivity (in mS/cm) = Conversion Factor * Diffusivity (in cm^2/s)
        """
        df_sp = get_el_sp(species)
        if hasattr(df_sp, "oxi_state"):
            z = df_sp.oxi_state
        else:
            z = df_sp.full_electronic_structure[-1][2]

        n = structure.composition[species]

        vol = structure.volume * 1e-24  # units cm^3
        return 1000 * n / (vol * const.N_A) * z ** 2 * (const.N_A * const.e) ** 2 / (const.R * temperature)

    def _get_vasprun(args):
        """
        Internal method to support multiprocessing.
        """
        return Vasprun(args[0], ionic_step_skip=args[1],
                       parse_dos=False, parse_eigen=False)

    def fit_arrhenius(temps, diffusivities):
        """
        Returns Ea, c, standard error of Ea from the Arrhenius fit:
            D = c * exp(-Ea/kT)

        Args:
            temps ([float]): A sequence of temperatures. units: K
            diffusivities ([float]): A sequence of diffusivities (e.g.,
                from DiffusionAnalyzer.diffusivity). units: cm^2/s
        """
        t_1 = 1 / np.array(temps)
        logd = np.log(diffusivities)
        # Do a least squares regression of log(D) vs 1/T
        a = np.array([t_1, np.ones(len(temps))]).T
        w, res, _, _ = np.linalg.lstsq(a, logd, rcond=None)
        w = np.array(w)
        n = len(temps)
        if n > 2:
            std_Ea = (res[0] / (n - 2) / (
                    n * np.var(t_1))) ** 0.5 * const.k / const.e
        else:
            std_Ea = None
        return -w[0] * const.k / const.e, np.exp(w[1]), std_Ea

    def get_extrapolated_diffusivity(temps, diffusivities, new_temp):
        """
        Returns (Arrhenius) extrapolated diffusivity at new_temp

        Args:
            temps ([float]): A sequence of temperatures. units: K
            diffusivities ([float]): A sequence of diffusivities (e.g.,
                from DiffusionAnalyzer.diffusivity). units: cm^2/s
            new_temp (float): desired temperature. units: K

        Returns:
            (float) Diffusivity at extrapolated temp in mS/cm.
        """
        Ea, c, _ = fit_arrhenius(temps, diffusivities)
        return c * np.exp(-Ea / (const.k / const.e * new_temp))

    def get_extrapolated_conductivity(temps, diffusivities, new_temp, structure,
                                      species):
        """
        Returns extrapolated mS/cm conductivity.

        Args:
            temps ([float]): A sequence of temperatures. units: K
            diffusivities ([float]): A sequence of diffusivities (e.g.,
                from DiffusionAnalyzer.diffusivity). units: cm^2/s
            new_temp (float): desired temperature. units: K
            structure (structure): Structure used for the diffusivity calculation
            species (string/Specie): conducting species

        Returns:
            (float) Conductivity at extrapolated temp in mS/cm.
        """
        return get_extrapolated_diffusivity(temps, diffusivities, new_temp) \
            * get_conversion_factor(structure, species, new_temp)

    def get_arrhenius_plot(temps, diffusivities, diffusivity_errors=None,
                           **kwargs):
        r"""
        Returns an Arrhenius plot.

        Args:
            temps ([float]): A sequence of temperatures.
            diffusivities ([float]): A sequence of diffusivities (e.g.,
                from DiffusionAnalyzer.diffusivity).
            diffusivity_errors ([float]): A sequence of errors for the
                diffusivities. If None, no error bar is plotted.
            \\*\\*kwargs:
                Any keyword args supported by matplotlib.pyplot.plot.

        Returns:
            A matplotlib.pyplot object. Do plt.show() to show the plot.
        """
        Ea, c, _ = fit_arrhenius(temps, diffusivities)

        from pymatgen.util.plotting import pretty_plot
        plt = pretty_plot(12, 8)

        # log10 of the arrhenius fit
        arr = c * np.exp(-Ea / (const.k / const.e * np.array(temps)))

        t_1 = 1000 / np.array(temps)

        plt.plot(t_1, diffusivities, 'ko', t_1, arr, 'k--', markersize=10,
                 **kwargs)
        if diffusivity_errors is not None:
            n = len(diffusivity_errors)
            plt.errorbar(t_1[0:n], diffusivities[0:n], yerr=diffusivity_errors,
                         fmt='ko', ecolor='k', capthick=2, linewidth=2)
        ax = plt.axes()
        ax.set_yscale('log')
        plt.text(0.6, 0.85, "E$_a$ = {:.0f} meV".format(Ea * 1000),
                 fontsize=30, transform=plt.axes().transAxes)
        plt.ylabel("D (cm$^2$/s)")
        plt.xlabel("1000/T (K$^{-1}$)")
        plt.tight_layout()
        return plt