Remove unused waveguide_mode functions
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d2d4220313
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@ -307,107 +307,6 @@ def solve_waveguide_mode_cylindrical(mode_number: int,
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return fields
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def compute_source_q(E: field_t,
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H: field_t,
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wavenumber: complex,
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omega: complex,
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dxes: dx_lists_t,
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axis: int,
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polarity: int,
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slices: List[slice],
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mu: field_t = None,
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) -> field_t:
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A1f = functional.curl_h(dxes)
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A2f = functional.curl_e(dxes)
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J = A1f(H)
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M = A2f(-E)
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m2j = functional.m2j(omega, dxes, mu)
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Jm = m2j(M)
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Jtot = J + Jm
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return Jtot, J, M
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def compute_source_e(QE: field_t,
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omega: complex,
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dxes: dx_lists_t,
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axis: int,
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polarity: int,
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slices: List[slice],
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epsilon: field_t,
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mu: field_t = None,
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) -> field_t:
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"""
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Want AQE = -iwJ, where Q is mask and normally AE = -iwJ
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## Want (AQ-QA) E = -iwJ, where Q is a mask
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## If E is an eigenmode, AE = 0 so just AQE = -iwJ
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Really only need E in 4 cells along axis (0, 0, Emode1, Emode2), find AE (1 iteration), then use center 2 cells as src
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Maybe better to use (0, Emode1, Emode2, Emode3), find AE (1 iteration), then use left 2 cells as src?
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"""
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slices = tuple(slices)
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# Trim a cell from each end of the propagation axis
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slices_reduced = list(slices)
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for aa in range(3):
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if aa == axis:
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if polarity > 0:
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slices_reduced[axis] = slice(slices[axis].start, slices[axis].start+2)
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else:
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slices_reduced[axis] = slice(slices[axis].stop-2, slices[axis].stop)
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else:
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start = slices[aa].start
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stop = slices[aa].stop
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# if start is not None or stop is not None:
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# if start is None:
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# start = 1
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# stop -= 1
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# elif stop is None:
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# stop = E.shape[aa + 1] - 1
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# start += 1
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# else:
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# start += 1
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# stop -= 1
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# slices_reduced[aa] = slice(start, stop)
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slices_reduced = (slice(None), *slices_reduced)
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# Don't actually need to mask out E here since it needs to be pre-masked (QE)
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A = functional.e_full(omega, dxes, epsilon, mu)
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J4 = A(QE) / (-1j * omega) #J4 is 4-cell result of -iwJ = A QE
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J = numpy.zeros_like(J4)
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J[slices_reduced] = J4[slices_reduced]
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return J
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def compute_source_wg(E: field_t,
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wavenumber: complex,
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omega: complex,
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dxes: dx_lists_t,
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axis: int,
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polarity: int,
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slices: List[slice],
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epsilon: field_t,
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mu: field_t = None,
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) -> field_t:
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slices = tuple(slices)
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Etgt, _slices2 = compute_overlap_ce(E=E, wavenumber=wavenumber,
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dxes=dxes, axis=axis, polarity=polarity,
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slices=slices)
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slices4 = list(slices)
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slices4[axis] = slice(slices[axis].start - 4 * polarity, slices[axis].start)
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slices4 = tuple(slices4)
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J = compute_source_e(QE=Etgt,
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omega=omega, dxes=dxes, axis=axis,
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polarity=polarity, slices=slices4,
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epsilon=epsilon, mu=mu)
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return J
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def compute_overlap_ce(E: field_t,
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wavenumber: complex,
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dxes: dx_lists_t,
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