from solcore.structure import Layer, Junction, TunnelJunction
from solcore.absorption_calculator import calculate_rat_rcwa, calculate_absorption_profile_rcwa
import numpy as np
import types
from solcore.state import State
rcwa_options = State()
rcwa_options.size = [500, 500]
rcwa_options.orders = 4
rcwa_options.theta = 0
rcwa_options.phi = 0
rcwa_options.pol = 'u'
def solve_rcwa(solar_cell, options):
""" Calculates the reflection, transmission and absorption of a solar cell object using the transfer matrix method
:param solar_cell:
:param options:
:return:
"""
wl = options.wavelength
# We include the shadowing losses
initial = (1 - solar_cell.shading) if hasattr(solar_cell, 'shading') else 1
# Now we calculate the absorbed and transmitted light. We first get all the relevant parameters from the objects
widths = []
offset = 0
all_layers = []
# And, finally, we put everything together, adding also the surface recombination velocities sn and sp.
# setting kind = 'DA' in the Junction definition tells the electrical solver later to use the depletion approximation
optical_struct = SolarCell(ARC + top_junction + middle_junction + DBRa + DBRb +
DBRc + bottom_junction,
shading=0.05)
wl = np.linspace(250, 1700, 400) * 1e-9
options = State()
options.wavelength = wl
options.optics_method = 'TMM'
options.no_back_reflection = False
options.pol = 'p'
options.BL_correction = True
options.coherency_list = 111 * ['c']
options.theta = 30
solar_cell_solver(optical_struct, 'qe', options)
plt.figure()
plt.plot(
wl * 1e9,
optical_struct[0].layer_absorption + optical_struct[1].layer_absorption)
plt.plot(wl * 1e9, optical_struct[2].layer_absorption)
plt.plot(wl * 1e9, optical_struct[3].layer_absorption)
plt.plot(wl * 1e9, optical_struct[100].layer_absorption)
plt.plot(wl * 1e9, optical_struct.absorbed, '--')
plt.plot(wl * 1e9, optical_struct.transmitted, '--')
plt.plot(wl * 1e9, optical_struct.reflected, '--')
plt.legend(['ARC', 'top', 'middle', 'bottom', 'A', 'T', 'R'])
plt.ylim(0, 1)
plt.ylabel('Absorption/Transmission/Reflection')