def theta_electric_i_te(radial,
theta,
phi,
wave_number_k,
degrees=[-1, 1],
bscs={}):
""" Computes the theta component of inciding electric field in TE mode.
"""
result = 0
n = 1
# Due to possible singularity near origin, we approximate null radial
# component to a small value.
radial = radial or 1E-16
riccati_bessel_list = _riccati_bessel_j(get_max_it(radial, wave_number_k),
wave_number_k * radial)
riccati_bessel = riccati_bessel_list[0]
max_it = get_max_it(radial, wave_number_k)
while n <= max_it:
for m in degrees:
if n >= m:
increment = m \
* plane_wave_coefficient(n, wave_number_k) \
* bscs[(n, m)] \
* riccati_bessel[n] \
* legendre_pi(n, abs(m), np.cos(theta)) \
* np.exp(1j * m * phi)
result += increment
n += 1
return result / radial
def radial_electric_i_tm(radial,
theta,
phi,
wave_number_k,
degrees=[-1, 1],
bscs={}):
""" Computes the radial component of incident electric field in TM mode.
"""
result = 0
n = 1
riccati_bessel_list = _riccati_bessel_j(get_max_it(radial, wave_number_k),
wave_number_k * radial)
riccati_bessel = riccati_bessel_list[0]
max_it = get_max_it(radial, wave_number_k)
# while n <= get_max_it(radial, wave_number_k):
while n <= max_it:
for m in degrees:
if n >= m:
increment = plane_wave_coefficient(n, wave_number_k) \
* bscs[(n, m)] \
* (d2_riccati_bessel_j(n, wave_number_k * radial)
+ riccati_bessel[n]) \
* legendre_p(n, abs(m), np.cos(theta)) \
* np.exp(1j * m * phi)
result += increment
n += 1
return wave_number_k * result