PEC and PMC for all wave operators
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@ -177,12 +177,18 @@ def test1():
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J = waveguide_mode.compute_source(**wg_args, **wg_results)
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H_overlap = waveguide_mode.compute_overlap_e(**wg_args, **wg_results)
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pecg = gridlock.Grid(edge_coords, initial=0, num_grids=3)
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pecg = gridlock.Grid(edge_coords, initial=0.0, num_grids=3)
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# pecg.draw_cuboid(center=[700, 0, 0], dimensions=[80, 1e8, 1e8], eps=1)
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pecg.grids = [numpy.sign(r) for r in pecg.grids]
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# pecg.visualize_isosurface()
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A = fdfd_tools.operators.e_full(omega, dxes, vec(grid.grids), pec=vec(pecg.grids)).tocsr()
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pmcg = gridlock.Grid(edge_coords, initial=0.0, num_grids=3)
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# pmcg.draw_cuboid(center=[700, 0, 0], dimensions=[80, 1e8, 1e8], eps=1)
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# pmcg.visualize_isosurface()
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A = fdfd_tools.operators.e_full(omega, dxes,
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epsilon=vec(grid.grids),
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pec=vec(pecg.grids),
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pmc=vec(pmcg.grids)).tocsr()
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b = -1j * omega * vec(J)
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x = solve_A(A, b)
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E = unvec(x, grid.shape)
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@ -47,6 +47,7 @@ def e_full(omega: complex,
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epsilon: vfield_t,
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mu: vfield_t = None,
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pec: vfield_t = None,
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pmc: vfield_t = None,
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) -> sparse.spmatrix:
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"""
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Wave operator del x (1/mu * del x) - omega**2 * epsilon, for use with E-field,
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@ -61,6 +62,8 @@ def e_full(omega: complex,
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:param mu: Vectorized magnetic permeability (default 1 everywhere).
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:param pec: Vectorized mask specifying PEC cells. Any cells where pec != 0 are interpreted
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as containing a perfect electrical conductor (PEC).
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:param pmc: Vectorized mask specifying PMC cells. Any cells where pmc != 0 are interpreted
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as containing a perfect magnetic conductor (PMC).
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:return: Sparse matrix containing the wave operator
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"""
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ce = curl_e(dxes)
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@ -68,10 +71,15 @@ def e_full(omega: complex,
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ev = epsilon
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if numpy.any(numpy.equal(pec, None)):
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pe = sparse.eye(epsilon.size)
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else:
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pe = sparse.diags(numpy.where(pec, 0, 1)) # Set pe to (not PEC)
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ev = numpy.where(pec, 1.0, ev) # Set epsilon to 1 at PEC
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if numpy.any(numpy.equal(pmc, None)):
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pm = sparse.eye(epsilon.size)
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else:
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pm = sparse.diags(numpy.where(pec, 0, 1)) # Set pm to (not PEC)
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ev = numpy.where(pec, 1.0, ev) # Set epsilon to 1 at PEC
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pm = sparse.diags(numpy.where(pmc, 0, 1)) # set pm to (not PMC)
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e = sparse.diags(ev)
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if numpy.any(numpy.equal(mu, None)):
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@ -79,7 +87,7 @@ def e_full(omega: complex,
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else:
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m_div = sparse.diags(1 / mu)
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op = pm @ ch @ m_div @ ce @ pm - omega**2 * e
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op = pe @ ch @ pm @ m_div @ ce @ pe - omega**2 * e
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return op
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@ -110,6 +118,7 @@ def h_full(omega: complex,
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dxes: dx_lists_t,
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epsilon: vfield_t,
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mu: vfield_t = None,
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pec: vfield_t = None,
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pmc: vfield_t = None,
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) -> sparse.spmatrix:
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"""
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@ -121,6 +130,8 @@ def h_full(omega: complex,
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:param dxes: Grid parameters [dx_e, dx_h] as described in fdfd_tools.operators header
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:param epsilon: Vectorized dielectric constant
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:param mu: Vectorized magnetic permeability (default 1 everywhere)
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:param pec: Vectorized mask specifying PEC cells. Any cells where pec != 0 are interpreted
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as containing a perfect electrical conductor (PEC).
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:param pmc: Vectorized mask specifying PMC cells. Any cells where pmc != 0 are interpreted
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as containing a perfect magnetic conductor (PMC).
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:return: Sparse matrix containing the wave operator
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@ -134,19 +145,24 @@ def h_full(omega: complex,
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mv = mu
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if numpy.any(numpy.equal(pmc, None)):
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pm = sparse.eye(epsilon.size)
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else:
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pm = sparse.diags(numpy.where(pmc, 0, 1)) # Set pe to (not PMC)
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mv = numpy.where(pmc, 1.0, mv) # Set mu to 1 at PMC
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if numpy.any(numpy.equal(pec, None)):
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pe = sparse.eye(epsilon.size)
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else:
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pe = sparse.diags(numpy.where(pmc, 0, 1)) # Set pe to (not PMC)
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mv = numpy.where(pmc, 1.0, mv) # Set mu to 1 at PMC
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pe = sparse.diags(numpy.where(pec, 0, 1)) # set pe to (not PEC)
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e_div = sparse.diags(1 / epsilon)
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m = sparse.diags(mv)
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A = pe @ ec @ e_div @ hc @ pe - omega**2 * m
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A = pm @ ec @ pe @ e_div @ hc @ pm - omega**2 * m
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return A
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def eh_full(omega, dxes, epsilon, mu=None):
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def eh_full(omega, dxes, epsilon, mu=None, pec=None, pmc=None):
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"""
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Wave operator for [E, H] field representation. This operator implements Maxwell's
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equations without cancelling out either E or H. The operator is
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@ -159,18 +175,32 @@ def eh_full(omega, dxes, epsilon, mu=None):
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:param dxes: Grid parameters [dx_e, dx_h] as described in fdfd_tools.operators header
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:param epsilon: Vectorized dielectric constant
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:param mu: Vectorized magnetic permeability (default 1 everywhere)
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:param pec: Vectorized mask specifying PEC cells. Any cells where pec != 0 are interpreted
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as containing a perfect electrical conductor (PEC).
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:param pmc: Vectorized mask specifying PMC cells. Any cells where pmc != 0 are interpreted
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as containing a perfect magnetic conductor (PMC).
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:return: Sparse matrix containing the wave operator
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"""
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A2 = curl_e(dxes)
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A1 = curl_h(dxes)
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if numpy.any(numpy.equal(pec, None)):
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pe = sparse.eye(epsilon.size)
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else:
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pe = sparse.diags(numpy.where(pec, 0, 1)) # set pe to (not PEC)
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iwe = 1j * omega * sparse.diags(epsilon)
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iwm = 1j * omega
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if numpy.any(numpy.equal(pmc, None)):
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pm = sparse.eye(epsilon.size)
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else:
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pm = sparse.diags(numpy.where(pmc, 0, 1)) # set pm to (not PMC)
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iwe = pe @ (1j * omega * sparse.diags(epsilon))
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iwm = pm * 1j * omega
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if not numpy.any(numpy.equal(mu, None)):
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iwm *= sparse.diags(mu)
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A1 = pe @ curl_h(dxes) @ pm
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A2 = pm @ curl_e(dxes) @ pe
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A = sparse.bmat([[-iwe, A1],
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[A2, +iwm]])
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[A2, iwm]])
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return A
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