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Use e_boundary_source for compute_source

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Jan Petykiewicz 2019-08-26 01:03:13 -07:00
parent 7b56aa363f
commit 5f96474497
1 changed files with 13 additions and 25 deletions
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38
meanas/fdfd/waveguide_mode.py
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@ -137,13 +137,13 @@ def solve_waveguide_mode(mode_number: int,
def compute_source(E: field_t, def compute_source(E: field_t,
H: field_t,
wavenumber: complex, wavenumber: complex,
omega: complex, omega: complex,
dxes: dx_lists_t, dxes: dx_lists_t,
axis: int, axis: int,
polarity: int, polarity: int,
slices: List[slice], slices: List[slice],
epsilon: field_t,
mu: field_t = None, mu: field_t = None,
) -> field_t: ) -> field_t:
""" """
@ -151,7 +151,6 @@ def compute_source(E: field_t,
necessary to position a unidirectional source at the slice location. necessary to position a unidirectional source at the slice location.
:param E: E-field of the mode :param E: E-field of the mode
:param H: H-field of the mode (advanced by half of a Yee cell from E)
:param wavenumber: Wavenumber of the mode :param wavenumber: Wavenumber of the mode
:param omega: Angular frequency of the simulation :param omega: Angular frequency of the simulation
:param dxes: Grid parameters [dx_e, dx_h] as described in meanas.types :param dxes: Grid parameters [dx_e, dx_h] as described in meanas.types
@ -162,32 +161,21 @@ def compute_source(E: field_t,
:param mu: Magnetic permeability (default 1 everywhere) :param mu: Magnetic permeability (default 1 everywhere)
:return: J distribution for the unidirectional source :return: J distribution for the unidirectional source
""" """
J = numpy.zeros_like(E, dtype=complex) E_expanded = expand_wgmode_e(E=E, dxes=dxes, wavenumber=wavenumber, axis=axis,
M = numpy.zeros_like(E, dtype=complex) polarity=polarity, slices=slices)
src_order = numpy.roll(range(3), -axis) smask = [slice(None)] * 4
if polarity > 0:
smask[axis + 1] = slice(slices[axis].start, None)
else:
smask[axis + 1] = slice(None, slices[axis].stop)
# exp_iphi = numpy.exp(1j * polarity * wavenumber * dxes[1][axis][slices[axis]]) mask = numpy.zeros_like(E_expanded, dtype=int)
# rollby = -1 if polarity > 0 else 0 mask[tuple(smask)] = 1
# J[src_order[1]] = +exp_iphi * H[src_order[2]] * polarity / dxes[1][axis][slices[axis]]
# J[src_order[2]] = -exp_iphi * H[src_order[1]] * polarity / dxes[1][axis][slices[axis]]
# M[src_order[1]] = +numpy.roll(E[src_order[2]], rollby, axis=axis) / dxes[0][axis][slices[axis]]
# M[src_order[2]] = -numpy.roll(E[src_order[1]], rollby, axis=axis) / dxes[0][axis][slices[axis]]
s2 = [slice(None), slice(None), slice(None)] masked_e2j = operators.e_boundary_source(mask=vec(mask), omega=omega, dxes=dxes, epsilon=vec(epsilon), mu=vec(mu))
s2[axis] = slice(slices[axis].start, slices[axis].stop) J = unvec(masked_e2j @ vec(E_expanded), E.shape[1:])
s2 = (src_order, *s2) return J
rollby = 1 if polarity < 0 else 0
exp_iphi = numpy.exp(-1j * -rollby * wavenumber * dxes[1][axis][slices[axis]])
J[s2] = numpy.roll(functional.curl_h(dxes=dxes)(H), -rollby, axis=axis+1)[s2] * exp_iphi * -polarity
M[s2] = numpy.roll(functional.curl_e(dxes=dxes)(E), rollby, axis=axis+1)[s2]
m2j = functional.m2j(omega, dxes, mu)
Jm = m2j(M)
Jtot = J + Jm
return Jtot
def compute_overlap_e(E: field_t, def compute_overlap_e(E: field_t,