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42 changes: 36 additions & 6 deletions femwell/maxwell/waveguide.py
Original file line number Diff line number Diff line change
Expand Up @@ -23,10 +23,12 @@
ElementTriP1,
ElementTriP2,
ElementVector,
FacetBasis,
Functional,
InteriorFacetBasis,
LinearForm,
Mesh,
bmat,
condense,
solve,
)
Expand Down Expand Up @@ -527,6 +529,7 @@ def compute_modes(
num_modes=1,
order=1,
metallic_boundaries=False,
surface_impedances={},
radius=np.inf,
n_guess=None,
solver="scipy",
Expand Down Expand Up @@ -602,11 +605,37 @@ def bform(e_t, e_z, v_t, v_z, w):
solver=solver(k=num_modes, sigma=sigma),
)
else:
lams, xs = solve(
-A,
-B,
solver=solver(k=num_modes, sigma=sigma),
)
if not surface_impedances:
lams, xs = solve(
-A,
-B,
solver=solver(k=num_modes, sigma=sigma),
)
else:

@BilinearForm(dtype=complex)
def cform(e_t, e_z, v_t, v_z, w):
return e_z * v_z

basis_facet = FacetBasis(basis.mesh, basis.elem)
C = cform.assemble(basis_facet)

@BilinearForm(dtype=complex)
def dform(e_t, e_z, v_t, v_z, w):
return 0.01 * curl(e_t) * 1j * v_z

basis_facet = FacetBasis(
basis.mesh, basis.elem, facets=basis.mesh.boundaries["core___clad"]
)
D = dform.assemble(basis_facet)

I = scipy.sparse.identity(A.shape[0])
lams, xs = solve(
bmat([[-A, None], [C, I]]),
bmat([[-B, None], [D, I]]),
solver=solver(k=num_modes, sigma=sigma),
)
xs = xs[: A.shape[0]]

xs[basis.split_indices()[1], :] /= 1j * np.sqrt(
lams[np.newaxis, :] / k0**4
Expand Down Expand Up @@ -896,7 +925,8 @@ def plot_mode(basis, mode, plot_vectors=False, colorbar=True, title="E", directi
mu_r=1,
num_modes=6,
order=2,
radius=3 * scale,
# radius=3 * scale,
surface_impedances={1: 2},
)
print(modes)
print(modes[0].te_fraction)
Expand Down
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