from solcore.constants import *
from numpy import array
import numpy as np
from solcore.science_tracker import science_reference
H = lambda x: 0 if x < 0 else 1 ### blindly changed this !!
D = lambda x, width: 1 if (x >= -width) and (x <= width) else 0 # Delta function
L = lambda x, centre, hwhm: 1 / pi * (0.5 * hwhm) / (
(x - centre) ** 2 + (0.5 * hwhm) ** 2) # Lorenzian (area normalised to 1)
Gauss = lambda x, centre, hwhm: 1 / np.sqrt(2 * pi) / (0.5 * hwhm) * np.exp(
-0.5 * (x - centre) ** 2 / (0.5 * hwhm) ** 2) # Gaussian (area normalised to 1)
[docs]def exciton_rydberg_energy_2d(me, mh, eps_r):
"""
:param me: electron effective mass (units: kg)
:param mh: hole effective mass (units: kg)
:param eps_r: dielectic constant (units: SI)
:return: The exciton Rydberg energy
"""
science_reference("Definition of the exciton Rydberg Energy for a quantum well.",
"S. L. Chuang, Physics of Optoelectonic Devices, Second Edition, p.554, Table 13.1")
mr = me * mh / (me + mh) # reduced effective mass
if True:
return mr * q ** 4 / (2 * hbar ** 2 * (4 * np.pi * eps_r * vacuum_permittivity) ** 2)
Ry = 13.6 * 1.6e-19
m0 = electron_mass
Ry_eff = (mr / m0) * Ry / eps_r ** 2 # Effective Rydberg
return Ry_eff
[docs]def exciton_bohr_radius(me, mh, eps):
"""
:param me: electron effective mass (units: kg)
:param mh: hole effective mass (units: kg)
:param eps: dielectic constant (units: SI)
:return: Exciton Borh radius
"""
science_reference("Definition of the exciton bohr radius for a quantum well.",
"S. L. Chuang, Physics of Optoelectonic Devices, Second Edition, p.554, Table 13.1")
mr = me * mh / (me + mh) # reduced effective mass
return hbar ** 2 / mr * (4 * np.pi * eps / q ** 2)
[docs]def alpha_c_hh_TE(E, z, E_e, E_hh, psi_e, psi_hh, well_width, me, mhh, Ep, nr):
""" Absortion coefficient for incident light forming a transision between hh and c band of a quantum well
NB. Assumes that valence band is a zero energy, might need to manually apply an offset.
:param E: photon energy (units: J)
:param z: mesh points along growth direction (units: m)
:param E_e: Electron state energy (units: J)
:param E_hh: Heavy hole state energy (units: J)
:param psi_e: Electron envelope function (psi_e^2 must be normalised)
:param psi_hh: Heavy hole envelope function (psi_hh^2 must be normalised)
:param well_width: (units: m)
:param me: electron effective mass (units: kg)
:param mhh: heavy hole effective mass (units: kg)
:param Ep: the Kane parameter "Optical dipole matrix elemet", sometimes "Momentum matrix element", e.g. Ep for GaAs ~ 28eV
:param nr: refractive index
:return:
"""
m0 = electron_mass
C0 = np.pi * q ** 2 / (nr * c * vacuum_permittivity * m0 ** 2 * E / hbar)
mr = me * mhh / (me + mhh) # reduced effective mass
DOS_2D = mr / (np.pi * hbar ** 2 * well_width)
Mbsq_3D = m0 / 6 * Ep
Mbsq_2D = 3 / 2 * Mbsq_3D
Ieh = np.trapz(psi_e * psi_hh, z) ** 2
return C0 * Ieh * Mbsq_2D * DOS_2D * H(E - (E_e - E_hh))
[docs]def alpha_c_lh_TE(E, z, E_e, E_lh, psi_e, psi_lh, well_width, me, mlh, Ep, nr):
""" Absortion coefficient for incident light forming a transision between hh and c band of a quantum well
NB. Assumes that valence band is a zero energy, might need to manually apply an offset.
:param E: photon energy (units: J)
:param z: mesh points along growth direction (units: m)
:param E_e: Electron state energy (units: J)
:param E_hh: Heavy hole state energy (units: J)
:param psi_e: Electron envelope function (psi_e^2 must be normalised)
:param psi_hh: Heavy hole envelope function (psi_hh^2 must be normalised)
:param well_width: (units: m)
:param me: electron effective mass (units: kg)
:param mhh: heavy hole effective mass (units: kg)
:param Ep: the Kane parameter "Optical dipole matrix elemet", sometimes "Momentum matrix element", e.g. Ep for GaAs ~ 28eV
:param nr: refractive index
:return:
"""
m0 = electron_mass
C0 = np.pi * q ** 2 / (nr * c * vacuum_permittivity * m0 ** 2 * E / hbar)
mr = me * mlh / (me + mlh) # reduced effective mass
DOS_2D = mr / (np.pi * hbar ** 2 * well_width)
Mbsq_3D = m0 / 6 * Ep
Mbsq_2D = 1 / 2 * Mbsq_3D
Ieh = np.trapz(psi_e * psi_lh, z) ** 2
return C0 * Ieh * Mbsq_2D * DOS_2D * H(E - (E_e - E_lh))
[docs]def alpha_exciton_ehh_TE(exciton_index, E, z, E_e, E_hh, psi_e, psi_hh, well_width, me, mhh, Ep, nr, eps,
hwhm=6e-3 * 1.6e-19, dimensionality=0.15, line_shape="Lorenzian"):
"""
:param exciton_index:
:param E:
:param z:
:param E_e:
:param E_hh:
:param psi_e:
:param psi_hh:
:param well_width:
:param me:
:param mhh:
:param Ep:
:param nr:
:param eps:
:param hwhm:
:param dimensionality:
:param line_shape:
:return:
"""
if exciton_index < 1:
raise ValueError("The excition index must start on 1.")
if dimensionality < 0 or dimensionality > 0.5:
raise ValueError("The dimensionality parameter of the exciton must be a number between 0 and 0.5 (inclusive).")
# Borrow constants from the bound-to-bound calculation
m0 = electron_mass
C0 = np.pi * q ** 2 / (nr * c * vacuum_permittivity * m0 ** 2 * E / hbar)
mr = me * mhh / (me + mhh) # reduced effective mass
DOS_2D = mr / (np.pi * hbar ** 2 * well_width)
Mbsq_3D = m0 / 6 * Ep
Mbsq_2D = 3 / 2 * Mbsq_3D
Ieh = np.trapz(psi_e * psi_hh, z) ** 2
# Excitions are considered by modiftying the bulk absorption coefficient using an oscillator strength
Ry_eff = exciton_rydberg_energy_2d(me, mhh, eps / vacuum_permittivity)
En = -Ry_eff / ((exciton_index - dimensionality) ** 2) # Exciton binding energy
Et = (E_e - E_hh)
# import pdb; pdb.set_trace()
# NOTE TO MARKUS: Added the possiblity of using a Gauss lineshape
if line_shape is "Gauss":
shape = Gauss(E, Et + En, hwhm)
else:
shape = L(E, Et + En, hwhm)
# NOTE TO MARKUS: It seems that there was a factor 2 missing in the oscilator strength as well as the exciton index.
# See: P C Klipstein and N Apsley 1986 J. Phys. C: Solid State Phys. 19 6461 doi:10.1088/0022-3719/19/32/020
oscillator_strength = (2 * Ry_eff / (exciton_index - dimensionality) ** 3)
return C0 * Ieh * Mbsq_2D * DOS_2D * oscillator_strength * shape
[docs]def alpha_exciton_elh_TE(exciton_index, E, z, E_e, E_lh, psi_e, psi_lh, well_width, me, mlh, Ep, nr, eps,
hwhm=6e-3 * 1.6e-19, dimensionality=0.15, line_shape="Lorenzian"):
"""
:param exciton_index:
:param E:
:param z:
:param E_e:
:param E_lh:
:param psi_e:
:param psi_lh:
:param well_width:
:param me:
:param mlh:
:param Ep:
:param nr:
:param eps:
:param hwhm:
:param dimensionality:
:param line_shape:
:return:
"""
if exciton_index < 1:
raise ValueError("The excition index must start on 1.")
if dimensionality < 0 or dimensionality > 0.5:
raise ValueError("The dimensionality parameter of the exciton must be a number between 0 and 0.5 (inclusive).")
# Borrow constants from the bound-to-bound calculation
m0 = electron_mass
C0 = np.pi * q ** 2 / (nr * c * vacuum_permittivity * m0 ** 2 * E / hbar)
mr = me * mlh / (me + mlh) # reduced effective mass
DOS_2D = mr / (np.pi * hbar ** 2 * well_width)
Mbsq_3D = m0 / 6 * Ep
Mbsq_2D = 1 / 2 * Mbsq_3D
Ieh = np.trapz(psi_e * psi_lh, z) ** 2
# Excitions are considered by modiftying the bulk absorption coefficient using an oscillator strength
Ry_eff = exciton_rydberg_energy_2d(me, mlh, eps / vacuum_permittivity)
En = -Ry_eff / ((exciton_index - dimensionality) ** 2) # Exciton binding energy
Et = (E_e - E_lh)
# NOTE TO MARKUS: Added the possiblity of using a Gauss lineshape
if line_shape is "Gauss":
shape = Gauss(E, Et + En, hwhm)
else:
shape = L(E, Et + En, hwhm)
# NOTE TO MARKUS: It seems that there was a factor 2 missing in the oscilator strength as well as the exciton index.
# See: P C Klipstein and N Apsley 1986 J. Phys. C: Solid State Phys. 19 6461 doi:10.1088/0022-3719/19/32/020
oscillator_strength = (2 * Ry_eff / (exciton_index - dimensionality) ** 3)
return C0 * Ieh * Mbsq_2D * DOS_2D * oscillator_strength * shape
[docs]def sum_alpha_c_hh_TE(E, z, E_e, E_hh, psi_e, psi_hh, well_width, me, mh, Ep, nr):
"""
:param E:
:param z:
:param E_e:
:param E_hh:
:param psi_e:
:param psi_hh:
:param well_width:
:param me:
:param mh:
:param Ep:
:param nr:
:return:
"""
alpha = 0
for ee, pe in zip(E_e, psi_e):
for eh, ph in zip(E_hh, psi_hh):
alpha += alpha_c_hh_TE(E, z, ee, eh, pe, ph, well_width, me, mh, Ep, nr)
return alpha
[docs]def sum_alpha_c_lh_TE(E, z, E_e, E_lh, psi_e, psi_lh, well_width, me, mh, Ep, nr):
"""
:param E:
:param z:
:param E_e:
:param E_lh:
:param psi_e:
:param psi_lh:
:param well_width:
:param me:
:param mh:
:param Ep:
:param nr:
:return:
"""
alpha = 0
for ee, pe in zip(E_e, psi_e):
for eh, ph in zip(E_lh, psi_lh):
alpha += alpha_c_lh_TE(E, z, ee, eh, pe, ph, well_width, me, mh, Ep, nr)
return alpha
[docs]def sum_alpha_exciton_c_hh_TE(E, z, E_e, E_hh, psi_e, psi_hh, well_width, me, mh, Ep, nr, eps, hwhm=6e-3 * 1.6e-19,
dimensionality=0.5, line_shape="Lorenzian"):
"""
:param E:
:param z:
:param E_e:
:param E_hh:
:param psi_e:
:param psi_hh:
:param well_width:
:param me:
:param mh:
:param Ep:
:param nr:
:param eps:
:param hwhm:
:param dimensionality:
:param line_shape:
:return:
"""
alpha = 0
eh_pairs_with_zero_angular_momentum = zip(range(len(E_e)),
range(len(E_hh))) # l=0 for optically allowed transitions
for exciton_index, eh_quantum_numbers in enumerate(eh_pairs_with_zero_angular_momentum):
e_index = eh_quantum_numbers[0]
hh_index = eh_quantum_numbers[1]
ee = E_e[e_index]
ehh = E_hh[hh_index]
pe = psi_e[e_index]
phh = psi_hh[e_index]
alpha += alpha_exciton_ehh_TE(exciton_index + 1, E, z, ee, ehh, pe, phh, well_width, me, mh, Ep, nr, eps,
hwhm=hwhm, dimensionality=dimensionality, line_shape=line_shape)
return alpha
[docs]def sum_alpha_exciton_c_lh_TE(E, z, E_e, E_lh, psi_e, psi_lh, well_width, me, mlh, Ep, nr, eps, hwhm=6e-3 * 1.6e-19,
dimensionality=0.5, line_shape="Lorenzian"):
"""
:param E:
:param z:
:param E_e:
:param E_lh:
:param psi_e:
:param psi_lh:
:param well_width:
:param me:
:param mlh:
:param Ep:
:param nr:
:param eps:
:param hwhm:
:param dimensionality:
:param line_shape:
:return:
"""
alpha = 0
eh_pairs_with_zero_angular_momentum = zip(range(len(E_e)),
range(len(E_lh))) # l=0 for optically allowed transitions
for exciton_index, eh_quantum_numbers in enumerate(eh_pairs_with_zero_angular_momentum):
e_index = eh_quantum_numbers[0]
lh_index = eh_quantum_numbers[1]
ee = E_e[e_index]
elh = E_lh[lh_index]
pe = psi_e[e_index]
plh = psi_lh[e_index]
alpha += alpha_exciton_elh_TE(exciton_index + 1, E, z, ee, elh, pe, plh, well_width, me, mlh, Ep, nr, eps,
hwhm=hwhm, dimensionality=dimensionality, line_shape=line_shape)
return alpha
[docs]def calc_alpha(QM_result, well_width, kane_parameter=28 * 1.6e-19, refractive_index=3.5, hwhm=6e-3 * 1.6e-19,
dimensionality=0.5, theta=0, eps=12.9 * vacuum_permittivity, espace=None, line_shape="Lorenzian"):
""" Calculates the absorption coeficient of a quantum well structure assuming the parabolic approximation for the
effective masses.
:param QM_result: The output of the Schrodinger solver, incldued in the 'quantum_mechanics' package
:param well_width: The well width
:param kane_parameter: The Kane parameter
:param refractive_index: Refractive (effective) index of the QW
:param hwhm: Full width at half maximum of the excitonic lineshape
:param dimensionality:
:param theta:
:param eps:
:param espace:
:param line_shape:
:return:
"""
results = QM_result
# We pick the effective mass at the center of the structure as THE efective mass of the QW
points = len(results["effective_masses"]["me"])
me = results["effective_masses"]["me"][round(points / 2.0)]
try:
mhh = results["effective_masses"]["mhh"][round(points / 2.0)]
mlh = results["effective_masses"]["mlh"][round(points / 2.0)]
except KeyError:
# If the calculation mode for the bands is kp4x4 or kp6x6, we have to use the effective mass transverse to the
# growth direction (in the QW plane).
mhh = results["effective_masses"]["mhh_t"][round(points / 2.0)]
mlh = results["effective_masses"]["mlh_t"][round(points / 2.0)]
# print (results["effective_masses"]["me"][round(points/2.0)])
# print (results["effective_masses"]["mhh"][round(points/2.0)])
# print (results["effective_masses"]["mlh"][round(points/2.0)])
result_c_hh_TE = []
result_c_lh_TE = []
result_ex_c_hh_TE = []
result_ex_c_lh_TE = []
for e in espace:
c_hh = sum_alpha_c_hh_TE(e, results['x'], results['E']['Ee'], results['E']['Ehh'],
results["wavefunctions"]['psi_e'], results["wavefunctions"]['psi_hh'], well_width, me,
mhh, kane_parameter, refractive_index)
c_lh = sum_alpha_c_lh_TE(e, results['x'], results['E']['Ee'], results['E']['Elh'],
results["wavefunctions"]['psi_e'], results["wavefunctions"]['psi_lh'], well_width, me,
mlh, kane_parameter, refractive_index)
ex_c_hh = sum_alpha_exciton_c_hh_TE(e, results['x'], results['E']['Ee'], results['E']['Ehh'],
results["wavefunctions"]['psi_e'], results["wavefunctions"]['psi_hh'],
well_width, me, mhh, kane_parameter, refractive_index, eps, hwhm=hwhm,
dimensionality=dimensionality, line_shape=line_shape)
ex_c_lh = sum_alpha_exciton_c_lh_TE(e, results['x'], results['E']['Ee'], results['E']['Elh'],
results["wavefunctions"]['psi_e'], results["wavefunctions"]['psi_lh'],
well_width, me, mlh, kane_parameter, refractive_index, eps, hwhm=hwhm,
dimensionality=dimensionality, line_shape=line_shape)
result_c_hh_TE.append(c_hh)
result_c_lh_TE.append(c_lh)
result_ex_c_hh_TE.append(ex_c_hh)
result_ex_c_lh_TE.append(ex_c_lh)
result_c_hh_TE = array(result_c_hh_TE)
result_c_lh_TE = array(result_c_lh_TE)
result_c_lh_TM = 4 * array(result_c_lh_TE)
result_ex_c_hh_TE = array(result_ex_c_hh_TE)
result_ex_c_lh_TE = array(result_ex_c_lh_TE)
result_ex_c_lh_TM = 4 * array(result_ex_c_lh_TE)
result_TE_raw = result_c_hh_TE + result_c_lh_TE + result_ex_c_hh_TE + result_ex_c_lh_TE
result_TE = result_TE_raw * (np.cos(theta) ** 2 + 0.5 * np.sin(theta) ** 2)
result_TM_raw = result_c_lh_TM + result_ex_c_lh_TM
result_TM = 0.5 * result_TM_raw * np.sin(theta) ** 2
result_sum = result_TE + result_TM
return espace, result_sum, result_TE, result_TM, result_TE_raw, result_TM_raw
[docs]def NonBlackBodyEmission(E, voltage=0, nr=3.5, T=300):
"""
:param E:
:param voltage:
:param nr:
:param T:
:return:
"""
A = 2 * nr ** 2 / h ** 3 / c ** 2
B = (E - q * voltage) / kb / T
bb = A * E ** 2 / (np.exp(B) - 1)
return bb
[docs]def calc_emission(QM_result, well_width, voltage=0, theta=0):
"""
:param QM_result:
:param well_width:
:param voltage:
:param theta:
:return:
"""
alfa = QM_result["alpha"]
aTE = alfa[4]
aTM = alfa[5]
result_TE = []
result_TM = []
result = []
for index, e in enumerate(alfa[0]):
bb = NonBlackBodyEmission(e)
TE = bb * (1 - np.exp(-aTE[index] * well_width * (np.cos(theta) ** 2 + 0.5 * np.sin(theta) ** 2)))
TM = bb * (1 - np.exp(-aTM[index] * well_width * 0.5 * np.sin(theta) ** 2))
# All = bb*(1-np.exp(-(aTE[index]+aTM[index])*well_width))
All = TE + TM
result_TE.append(TE)
result_TM.append(TM)
result.append(All)
result_TE = array(result_TE)
result_TM = array(result_TM)
result = array(result)
return alfa[0], result, result_TE, result_TM
