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Copy file name to clipboardExpand all lines: src/emscatter.jl
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# In this tutorial, we will learn:
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# * How to formulate the weak form for a scalar time-harmonic electromagnetic problem
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# * How to implement perfectly matched layers (PML)
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# * How does periodic boundary condition work in Gridap
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# * How to discretize PDEs with complex-valued solution
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# * How to implement a perfectly matched layer (PML) to absorb outgoing waves
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# * How to impose periodic boundary conditions in Gridap
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# * How to discretize PDEs with complex-valued solutions
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# ## Problem statement
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# We are going to solve a scalar electromagnetic wave scattering problem: a plane wave (Hz-polarized $H_{inc}$) scattering of a cylinder dielectric (of radius $R$ and permittivity $\varepsilon$), as illustrated below. The computational cell is of height $H$ and length $L$, and we designate a perfectly matched layer (PML) thickness of $d_{pml}$.
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# We are going to solve a scalar electromagnetic wave scattering problem: a plane wave (Hz-polarized $H_{inc}$) scattering of a dielectric cylinder (of radius $R$ and permittivity $\varepsilon$), as illustrated below. The computational cell is of height $H$ and length $L$, and we employ a perfectly matched layer (PML) thickness of $d_{pml}$ to implement outgoing (radiation) boundary conditions for this finite domain.
# [3] A. Oskooi and S. G. Johnson, “Distinguishing correct from incorrect PML proposals and a corrected unsplit PML for anisotropic, dispersive media,” Journal of Computational Physics, vol. 230, pp. 2369–2377, April 2011.
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# [3] A. Oskooi and S. G. Johnson, “[Distinguishing correct from incorrect PML proposals and a corrected unsplit PML for anisotropic, dispersive media](http://math.mit.edu/~stevenj/papers/OskooiJo11.pdf),” Journal of Computational Physics, vol. 230, pp. 2369–2377, April 2011.
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# [4] Stratton, J. A. (1941). Electromagnetic Theory. New York: McGraw-Hill.
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