use asarray() in place of array(copy=False)
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@ -88,7 +88,7 @@ def cg(
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def load_field(v: NDArray[numpy.complexfloating], dtype: type = numpy.complex128) -> pyopencl.array.Array:
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return pyopencl.array.to_device(queue, v.astype(dtype))
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r = load_field(b)
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r = load_field(numpy.asarray(b))
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x = pyopencl.array.zeros_like(r)
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v = pyopencl.array.zeros_like(r)
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p = pyopencl.array.zeros_like(r)
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@ -70,7 +70,7 @@ def cg_solver(
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shape = [dd.size for dd in dxes[0]]
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b = -1j * omega * numpy.array(J, copy=False)
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b = -1j * omega * numpy.asarray(J)
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'''
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** In this comment, I use the following notation:
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@ -99,7 +99,8 @@ def cg_solver(
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We can accomplish all this simply by conjugating everything (except J) and
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reversing the order of L and R
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'''
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epsilon = numpy.array(epsilon, copy=False)
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epsilon = numpy.asarray(epsilon)
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if adjoint:
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# Conjugate everything
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dxes = [[numpy.conj(dd) for dd in dds] for dds in dxes]
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@ -133,26 +134,26 @@ def cg_solver(
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rho = 1.0 + 0j
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errs = []
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inv_dxes = [[load_field(1 / numpy.array(dd, copy=False)) for dd in dds] for dds in dxes]
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oeps = load_field(-omega ** 2 * epsilon)
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inv_dxes = [[load_field(1 / numpy.asarray(dd)) for dd in dds] for dds in dxes]
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oeps = load_field(-omega * omega * epsilon)
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Pl = load_field(L.diagonal())
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Pr = load_field(R.diagonal())
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if mu is None:
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invm = load_field(numpy.array([]))
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else:
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invm = load_field(1 / numpy.array(mu, copy=False))
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mu = numpy.array(mu, copy=False)
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invm = load_field(1 / numpy.asarray(mu))
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mu = numpy.asarray(mu)
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if pec is None:
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gpec = load_field(numpy.array([]), dtype=numpy.int8)
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else:
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gpec = load_field(numpy.array(pec, dtype=bool, copy=False), dtype=numpy.int8)
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gpec = load_field(numpy.asarray(pec, dtype=bool), dtype=numpy.int8)
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if pmc is None:
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gpmc = load_field(numpy.array([]), dtype=numpy.int8)
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else:
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gpmc = load_field(numpy.array(pmc, dtype=bool, copy=False), dtype=numpy.int8)
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gpmc = load_field(numpy.asarray(pmc, dtype=bool), dtype=numpy.int8)
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'''
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Generate OpenCL kernels
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