Source code for qha.multi_configurations.same_phonon_dos

#!/usr/bin/env python3
"""
.. module multi_configurations.same_phonon_dos
   :platform: Unix, Windows, Mac, Linux
.. moduleauthor:: Qi Zhang <qz2280@columbia.edu>
"""

from typing import Optional

import numpy as np
from lazy_property import LazyProperty
from scipy.constants import physical_constants as pc
from scipy.special import logsumexp

import qha.settings
from qha.statmech import ho_free_energy, log_subsystem_partition_function
from qha.tools import calibrate_energy_on_reference
from qha.type_aliases import Array3D, Scalar, Vector, Matrix

# ===================== What can be exported? =====================
__all__ = ['PartitionFunction', 'FreeEnergy']

K = {'ha': pc['Boltzmann constant in eV/K'][0] / pc['Hartree energy in eV'][0],
     'ry': pc['Boltzmann constant in eV/K'][0] / pc['Rydberg constant times hc in eV'][0],
     'ev': pc['Boltzmann constant in eV/K'][0],
     'SI': pc['Boltzmann constant'][0]}[qha.settings.energy_unit]


[docs]class PartitionFunction: """ A class that represents the partition function of multiple configurations with the same phonon density of states. In mathematics, it is represented as .. math:: Z_{\\text{all configs}}(T, V) = \\sum_{j = 1}^{N_{c}} g_{j} \\bigg\\{ \\exp \\Big( -\\frac{ E_j(V) }{ k_B T } \\Big) \\prod_{\\mathbf{q}s} \\bigg( \\tfrac{\\exp \\big(-\\tfrac{ \\hbar \\omega_{\\mathbf{ q }s}^j(V) }{ 2 k_B T }\\big)}{1 - \\exp \\big(-\\tfrac{ \\hbar \\omega_{\\mathbf{ q }s}^j(V) }{ k_B T }\\big)} \\bigg)^{w_{\\mathbf{ q }}^j} \\bigg\\}. :param temperature: The temperature at which the partition function is calculated. :param degeneracies: An array of degeneracies of each configuration, which will not be normalized in the calculation. They should all be positive integers. :param q_weights: The weights of all q-points that are sampled, should be a vector since all configurations should have the same q-point weights. :param static_energies: The static energies of each configuration of each volume. :param frequencies: It is a 3D array that specifies the frequency on each volume, q-point and mode. It is not 4D since we have all configurations sharing the same phonon density of states. :param precision: The precision of a big float number to represent the partition function since it is a very large value, by default, is ``500``. """ def __init__(self, temperature: Scalar, degeneracies: Vector, q_weights: Vector, static_energies: Matrix, frequencies: Array3D, precision: Optional[int] = 500): if not np.all(np.greater_equal(degeneracies, 0)): raise ValueError('Degeneracies should all be integers greater equal than 0!') if not np.all(np.greater_equal(q_weights, 0)): # Weights should all be greater equal than 0, otherwise sum will be wrong. raise ValueError('Weights should all be greater equal than 0!') self.frequencies = np.array(frequencies) if self.frequencies.ndim != 3: raise ValueError("*frequencies* must be a three-dimensional array!") if temperature < 1e-6: self.temperature = 1e-6 else: self.temperature = temperature self.static_energies = np.array(static_energies) self.degeneracies = np.array(degeneracies) self.q_weights = np.array(q_weights) self._scaled_q_weights = self.q_weights / np.sum(q_weights) self.precision = int(precision) @property def _static_part(self) -> Vector: """ Calculate the static contribution to the partition function. :return: The static contribution on the temperature-volume grid. """ try: import mpmath except ImportError: raise ImportError( "You need to install ``mpmath`` package to use {0} object!".format(self.__class__.__name__)) with mpmath.workprec(self.precision): return np.array([mpmath.exp(d) for d in # shape = (# of volumes for each configuration, 1) logsumexp(-self.static_energies / (K * self.temperature), axis=1, b=self.degeneracies)]) @property def _harmonic_part(self) -> Vector: """ Calculate the harmonic contribution to the partition function. :return: The harmonic contribution on the temperature-volume grid. """ log_product_modes: Matrix = np.sum( log_subsystem_partition_function(self.temperature, self.frequencies), axis=2, dtype=float) return np.exp(np.dot(log_product_modes, self._scaled_q_weights)) # (vol, 1)
[docs] @LazyProperty def total(self) -> Vector: """ Calculate the total partition function. :return: The partition function on the temperature-volume grid. """ return np.multiply(self._static_part, self._harmonic_part) # (vol, 1), product element-wise
[docs] def get_free_energies(self): """ Give the free energy by .. math:: F_{\\text{all configs}}(T, V) = - k_B T \\ln Z_{\\text{all configs}}(T, V). :return: The free energy on the temperature-volume grid. """ try: import mpmath except ImportError: raise ImportError("Install ``mpmath`` package to use {0} object!".format(self.__class__.__name__)) with mpmath.workprec(self.precision): log_z = np.array([mpmath.log(d) for d in self.total], dtype=float) return -K * self.temperature * log_z
[docs]class FreeEnergy: """ A class that represents the free energy of multiple configurations with the same phonon density of states. In mathematics, it is represented as .. math:: F_{\\text{all configs}}(T, V) = - k_B T \\ln Z_{\\text{all configs}}(T, V) = - k_B T \\ln \\bigg( \\sum_{j = 1}^{N_{c}} g_{j} \\exp \\Big( -\\frac{ E_j(V) }{ k_B T } \\Big) \\bigg) + \\sum_{\\mathbf{ q }s} w_\\mathbf{ q } \\bigg\\{ \\frac{ \\hbar \\omega_{\\mathbf{ q }s}(V) }{ 2 } + k_B \\ln \\bigg( 1 - \\exp \\Big( -\\frac{ \\hbar \\omega_{\\mathbf{ q }s}(V) }{ k_B T } \\Big) \\bigg) \\bigg\\}. :param temperature: The temperature at which the partition function is calculated. :param degeneracies: An array of degeneracies of each configuration, which will not be normalized in the calculation. They should all be positive integers. :param q_weights: The weights of all q-points that are sampled, should be a vector since all configurations should have the same q-point weights. :param static_energies: The static energy of each configuration of each volume. :param volumes: A matrix of volumes of each configurations, should have the same values for each configuration. :param frequencies: It is a 3D array that specifies the frequency on each volume, q-point and mode. It is not 4D since we have all configurations sharing the same phonon density of states. :param static_only: Whether the calculation only takes static contribution and does not consider the vibrational contribution, by default, is ``False``. :param order: The order of Birch--Murnaghan equation of state fitting, by default, is ``3``. """ def __init__(self, temperature: Scalar, degeneracies: Vector, q_weights: Vector, static_energies: Matrix, volumes: Matrix, frequencies: Array3D, static_only: Optional[bool] = False, order: Optional[int] = 3): if not np.all(np.greater_equal(degeneracies, 0)): raise ValueError('Degeneracies should all be integers greater equal than 0!') if not np.all(np.greater_equal(q_weights, 0)): # Weights should all be greater equal than 0, otherwise sum will be wrong. raise ValueError('Weights should all be greater equal than 0!') self.frequencies = np.array(frequencies) if self.frequencies.ndim != 3: raise ValueError("*frequencies* must be a three-dimensional array!") if temperature < 1e-6: self.temperature = 1e-6 else: self.temperature = temperature self.static_energies = np.array(static_energies) self.volumes = np.array(volumes) self.degeneracies = np.array(degeneracies) self.q_weights = np.array(q_weights) self._scaled_q_weights = self.q_weights / np.sum(q_weights) self.static_only = static_only self.order = order
[docs] @LazyProperty def aligned_static_energies_for_each_configuration(self): """ If the input static energies are not aligned for each configuration, then do a fitting to align all static energies. :return: A matrix of aligned static energy of each configuration of each volume. """ return calibrate_energy_on_reference(self.volumes, self.static_energies, self.order)
[docs] @LazyProperty def static_part(self) -> Vector: """ Calculate the static contribution to the free energy. :return: The static contribution on the temperature-volume grid. """ kt: float = K * self.temperature # k_B T inside_exp: Matrix = -self.aligned_static_energies_for_each_configuration.T / kt # exp( E_n(V) / k_B / T ) return -kt * logsumexp(inside_exp, axis=1, b=self.degeneracies)
[docs] @LazyProperty def harmonic_part(self) -> Vector: """ Calculate the harmonic contribution to the free energy. :return: The harmonic contribution on the temperature-volume grid. """ sum_modes = np.sum(ho_free_energy(self.temperature, self.frequencies), axis=2) return np.dot(sum_modes, self._scaled_q_weights)
[docs] @LazyProperty def total(self) -> Vector: """ Calculate the total partition function, which is the static part plus the harmonic part. :return: Total free energy on the temperature-volume grid. """ return self.static_part + self.harmonic_part
[docs] def get_free_energies(self): """ If ``static_only = True`` is specified in class instantiation, then only the static contribution will be counted. Then it is equivalent to the ``static_part`` property. If not, then this is equivalent to the ``total`` property. :return: The free energy on the temperature-volume grid. """ if self.static_only: return self.static_part return self.total