Return: -> Returns:
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@ -29,7 +29,7 @@ def e_full(omega: complex,
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epsilon: Dielectric constant
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mu: Magnetic permeability (default 1 everywhere)
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Return:
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Returns:
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Function `f` implementing the wave operator
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`f(E)` -> `-i * omega * J`
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"""
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@ -99,7 +99,7 @@ def e2h(omega: complex,
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dxes: Grid parameters `[dx_e, dx_h]` as described in `meanas.fdmath.types`
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mu: Magnetic permeability (default 1 everywhere)
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Return:
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Returns:
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Function `f` for converting `E` to `H`,
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`f(E)` -> `H`
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"""
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@ -603,7 +603,7 @@ def curl_e(wavenumber: complex, dxes: dx_lists_t) -> sparse.spmatrix:
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wavenumber: Wavenumber assuming fields have z-dependence of `exp(-i * wavenumber * z)`
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dxes: Grid parameters `[dx_e, dx_h]` as described in `meanas.fdmath.types` (2D)
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Return:
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Returns:
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Sparse matrix representation of the operator.
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"""
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n = 1
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@ -623,7 +623,7 @@ def curl_h(wavenumber: complex, dxes: dx_lists_t) -> sparse.spmatrix:
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wavenumber: Wavenumber assuming fields have z-dependence of `exp(-i * wavenumber * z)`
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dxes: Grid parameters `[dx_e, dx_h]` as described in `meanas.fdmath.types` (2D)
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Return:
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Returns:
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Sparse matrix representation of the operator.
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"""
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n = 1
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