def get_thermodynamic_Gruneisen_parameter(gammas, frequencies, multiplicities,
t):
if t > 0:
cv = mode_cv(t, frequencies * THzToEv)
return (np.dot(multiplicities, cv * gammas).sum() /
np.dot(multiplicities, cv).sum())
else:
return 0.
def get_thermal_expansion_coefficient(gammas,
frequencies,
multiplicities,
t):
if t > 0:
return np.dot(multiplicities,
mode_cv(t, frequencies * THzToEv) * gammas).sum()
else:
return 0.
def get_thermal_expansion_coefficient(gammas,
frequencies,
multiplicities,
t):
if t > 0:
return np.dot(multiplicities,
mode_cv(t, frequencies * THzToEv) * gammas).sum()
else:
return 0.
def get_thermodynamic_Gruneisen_parameter(gammas,
frequencies,
multiplicities,
t):
if t > 0:
cv = mode_cv(t, frequencies * THzToEv)
return (np.dot(multiplicities, cv * gammas).sum() /
np.dot(multiplicities, cv).sum())
else:
return 0.
def get_thermodynamic_Gruneisen_parameter(gammas, frequencies, multiplicities,
t):
if t > 0:
conditions = (frequencies > 0)
freq_temp = np.where(conditions, x, 1)
cv_temp = mode_cv(t, frequencies * THzToEv)
cv = np.where(conditions, x, 0)
return (np.dot(multiplicities, cv * gammas).sum() /
np.dot(multiplicities, cv).sum())
else:
return 0.
def get_thermodynamic_Gruneisen_parameter(gammas,
frequencies,
multiplicities,
t):
if t > 0:
conditions = (frequencies > 0)
freq_temp = np.where(conditions, x, 1)
cv_temp = mode_cv(t, frequencies * THzToEv)
cv = np.where(conditions, x, 0)
return (np.dot(multiplicities, cv * gammas).sum() /
np.dot(multiplicities, cv).sum())
else:
return 0.
def mode_cv_matrix(temp, freqs, cutoff=1e-4):
r"""Calculate mode heat capacity matrix, Cqjj'.
C_{\mathbf{q}jj'} = K_B \frac{e^{x_{\mathbf{q}j} - x_{\mathbf{q}j'}} - 1}
{x_{\mathbf{q}j} - x_{\mathbf{q}j'}} \left( \frac{
x_{\mathbf{q}j} + x_{\mathbf{q}j'}}{2}
\right)^2 n_{\mathbf{q}j}(n_{\mathbf{q}j'} + 1)
Note
----
Diagonal (j=j') terms reduce to normal mode heat capacity.
Parameters
----------
temp : float
Temperature in K.
freqs : ndarray
Phonon frequencies at a q-point in eV.
cutoff : float
This is used to check the degeneracy.
Returns
-------
ndarray
Heat capacity matrix in eV/K.
shape=(num_band, num_band), dtype='double', order='C'.
"""
x = freqs / Kb / temp
shape = (len(freqs), len(freqs))
cvm = np.zeros(shape, dtype="double", order="C")
for i, j in np.ndindex(shape):
if abs(freqs[i] - freqs[j]) < cutoff:
cvm[i, j] = mode_cv(temp, freqs[i])
continue
sub = x[i] - x[j]
add = x[i] + x[j]
n_inv = np.exp([x[i], x[j], sub]) - 1
cvm[i, j] = Kb * n_inv[2] / sub * (add / 2) ** 2 / n_inv[0] * (1 / n_inv[1] + 1)
return cvm
def get_thermodynamic_Gruneisen_parameter(gammas, frequencies, t):
if t > 0:
cv = mode_cv(t, frequencies * THzToEv)
return np.sum(gammas * cv) / np.sum(cv)
else:
return 0.
def kappa_separate(self, gamma, thetaD, T, P=1, m=3, n=1):
"""
nkpts: number of phonon k-points
frequencies: list of eigenvalue-arrays as output by phonopy
vgroup: group velocities
T: temperature in K
following parameters from Eq (70) in Tritt book, p.14
P: proportionality factor of Umklapp scattering rate, defualt 1
mass: mass in amu (average mass of unitcell)
gamma: Gruneisen parameter, unitless
thetaD: Debye temperature of relevance (acoustic modes) 283K for Mo3Sb7
m = 3 by default
n = 1 by default
cellvol: unit cell volume in A^3
"""
T = float(T)
#self.phonon.set_mesh(mesh, is_eigenvectors=True)
#self.mass = self.phonon.get_primitive().get_masses().sum()/self.phonon.get_primitive().get_number_of_atoms()
self.cellvol = self.phonon.get_primitive().get_volume()
self.qpoints, self.weigths, self.frequencies, self.eigvecs = self.phonon.get_mesh(
)
nkpts = self.frequencies.shape[0]
numbranches = self.frequencies.shape[1]
self.group_velocity = np.zeros((nkpts, numbranches, 3))
for i in range(len(self.qpoints)):
self.group_velocity[i, :, :] = self.phonon.get_group_velocity_at_q(
self.qpoints[i])
inv_nor_Um = np.zeros((nkpts, numbranches))
inv_point_defect_mass_fc = np.zeros((nkpts, numbranches))
inv_tau_total = np.zeros((nkpts, numbranches))
kappa_Um = np.zeros((nkpts, numbranches))
kappa_point_defect_mass_fc = np.zeros((nkpts, numbranches))
kappa_total = np.zeros((nkpts, numbranches))
self.kappaten = np.zeros((nkpts, numbranches, 3, 3))
v_group = np.zeros((nkpts, numbranches))
capacity = np.zeros((nkpts, numbranches))
for i in range(nkpts):
for j in range(numbranches):
nu = self.frequencies[i][
j] # frequency (in Thz) of current mode
velocity = self.group_velocity[
i, j, :] # cartesian vector of group velocity
v_group = (velocity[0]**2 + velocity[1]**2 +
velocity[2]**2)**(0.5) * THztoA
capacity[i, j] = mode_cv(
T, nu * THzToEv) * eV2Joule / (self.cellvol * Ang2meter**3)
# tau inverse phonon-phonon, inverse lifetime
inv_nor_Um[i, j] = P * hbar * gamma**2 / (
self.mass * amu) / v_group**2 * (T**n) / thetaD * (
2 * np.pi * THz * nu)**2 * np.exp(
(-1.0) * thetaD / m / T)
# tau inverse point defect, inverse lifetime
inv_point_defect_mass_fc[i, j] = (self.mass_fc_factor) * (
2 * np.pi * THz * nu)**4 / v_group**3
# tau inverst, inverse lifetime
inv_tau_total[
i, j] = inv_nor_Um[i, j] + inv_point_defect_mass_fc[i, j]
kappa_total[
i,
j] = (1.0 / 3.0) * self.weigths[i] * v_group**2 * capacity[
i,
j] / inv_tau_total[i,
j] # 1/3 is for isotropic condition
kappa_Um[
i,
j] = (1.0 / 3.0) * self.weigths[i] * v_group**2 * capacity[
i, j] / inv_nor_Um[i,
j] # 1/3 is for isotropic condition
kappa_point_defect_mass_fc[
i,
j] = (1.0 / 3.0) * self.weigths[i] * v_group**2 * capacity[
i, j] / inv_point_defect_mass_fc[
i, j] # 1/3 is for isotropic condition
self.kappaten[i, j, :, :] = self.weigths[i] * np.outer(
velocity,
velocity) * THztoA**2 * capacity[i, j] / inv_tau_total[i,
j]
#print(np.sum(inv_nor_Um, axis =1))
#print(np.sum(inv_point_defect_mass_fc, axis =1))
#print(np.sum(inv_tau_total, axis =1))
self.tau = np.concatenate(
(inv_nor_Um, inv_point_defect_mass_fc, inv_tau_total), axis=1)
self.kappa = [
kappa_Um.sum() / self.weigths.sum(),
kappa_point_defect_mass_fc.sum() / self.weigths.sum(),
kappa_total.sum() / self.weigths.sum()
]
return self.tau, self.kappa, self.kappaten
def get_thermodynamic_Gruneisen_parameter(gammas, frequencies, t):
if t > 0:
cv = mode_cv(t, frequencies * THzToEv)
return np.sum(gammas * cv) / np.sum(cv)
else:
return 0.
