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ignore some lint

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This commit is contained in:
Forgejo Actions 2026-04-21 21:20:34 -07:00
commit a1568a6f16
6 changed files with 30 additions and 24 deletions
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8
meanas/fdfd/bloch.py
View file

@ -262,7 +262,7 @@ def maxwell_operator(
else:
# transform from mn to xyz
b_xyz = (m * b_m
+ n * b_n) # noqa: E128
+ n * b_n) # noqa
# divide by mu
temp = ifftn(b_xyz, axes=range(3))
@ -409,7 +409,7 @@ def inverse_maxwell_operator_approx(
else:
# transform from mn to xyz
h_xyz = (m * hin_m
+ n * hin_n) # noqa: E128
+ n * hin_n) # noqa
# multiply by mu
temp = ifftn(h_xyz, axes=range(3))
@ -474,7 +474,7 @@ def find_k(
`(k, actual_frequency, eigenvalues, eigenvectors)`
The found k-vector and its frequency, along with all eigenvalues and eigenvectors.
"""
direction = numpy.array(direction) / norm(direction)
direction = numpy.array(direction) / norm(direction) # type: ignore[operator]
k_bounds = tuple(sorted(k_bounds)) # type: ignore # we know the length already...
assert len(k_bounds) == 2
@ -504,7 +504,7 @@ def find_k(
assert n is not None
assert v is not None
actual_frequency = get_f(float(res.x), band)
return direction * float(res.x), float(actual_frequency), n, v
return direction * float(res.x), float(actual_frequency), n, v # type: ignore[operator,return-value]
def eigsolve(

12
meanas/fdfd/farfield.py
View file

@ -87,14 +87,14 @@ def near_to_farfield(
# Normalized vector potentials N, L
N = [-Hn_fft[1] * cos_phi * cos_th + Hn_fft[0] * cos_phi * sin_th,
Hn_fft[1] * sin_th + Hn_fft[0] * cos_th] # noqa: E127
Hn_fft[1] * sin_th + Hn_fft[0] * cos_th] # noqa
L = [ En_fft[1] * cos_phi * cos_th - En_fft[0] * cos_phi * sin_th,
-En_fft[1] * sin_th - En_fft[0] * cos_th] # noqa: E128
-En_fft[1] * sin_th - En_fft[0] * cos_th] # noqa
E_far = [-L[1] - N[0],
L[0] - N[1]] # noqa: E127
L[0] - N[1]] # noqa
H_far = [-E_far[1],
E_far[0]] # noqa: E127
E_far[0]] # noqa
theta = numpy.arctan2(ky, kx)
phi = numpy.arccos(cos_phi)
@ -203,9 +203,9 @@ def far_to_nearfield(
# Normalized vector potentials N, L
L = [0.5 * E_far[1],
-0.5 * E_far[0]] # noqa: E128
-0.5 * E_far[0]] # noqa
N = [L[1],
-L[0]] # noqa: E128
-L[0]] # noqa
En_fft = [
numpy.divide(

12
meanas/fdfd/waveguide_2d.py
View file

@ -373,8 +373,10 @@ def normalized_fields_e(
"""
e = exy2e(wavenumber=wavenumber, dxes=dxes, epsilon=epsilon) @ e_xy
h = exy2h(wavenumber=wavenumber, omega=omega, dxes=dxes, epsilon=epsilon, mu=mu) @ e_xy
e_norm, h_norm = _normalized_fields(e=e, h=h, omega=omega, dxes=dxes, epsilon=epsilon,
mu=mu, prop_phase=prop_phase)
e_norm, h_norm = _normalized_fields( # type: ignore[call-arg]
e=e, h=h, omega=omega, dxes=dxes, epsilon=epsilon,
mu=mu, prop_phase=prop_phase,
)
return e_norm, h_norm
@ -415,8 +417,10 @@ def normalized_fields_h(
"""
e = hxy2e(wavenumber=wavenumber, omega=omega, dxes=dxes, epsilon=epsilon, mu=mu) @ h_xy
h = hxy2h(wavenumber=wavenumber, dxes=dxes, mu=mu) @ h_xy
e_norm, h_norm = _normalized_fields(e=e, h=h, omega=omega, dxes=dxes, epsilon=epsilon,
mu=mu, prop_phase=prop_phase)
e_norm, h_norm = _normalized_fields( # type: ignore[call-arg]
e=e, h=h, omega=omega, dxes=dxes, epsilon=epsilon,
mu=mu, prop_phase=prop_phase,
)
return e_norm, h_norm

6
meanas/fdfd/waveguide_cyl.py
View file

@ -529,8 +529,10 @@ def normalized_fields_e(
"""
e = exy2e(angular_wavenumber=angular_wavenumber, omega=omega, dxes=dxes, rmin=rmin, epsilon=epsilon) @ e_xy
h = exy2h(angular_wavenumber=angular_wavenumber, omega=omega, dxes=dxes, rmin=rmin, epsilon=epsilon, mu=mu) @ e_xy
e_norm, h_norm = _normalized_fields(e=e, h=h, omega=omega, dxes=dxes, rmin=rmin, epsilon=epsilon,
mu=mu, prop_phase=prop_phase)
e_norm, h_norm = _normalized_fields( # type: ignore[call-arg]
e=e, h=h, omega=omega, dxes=dxes, rmin=rmin, epsilon=epsilon,
mu=mu, prop_phase=prop_phase,
)
return e_norm, h_norm