Difference between revisions of "Diffraction grating"

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== Additional information ==
 
== Additional information ==
  
To run the model, open '''grating2d.pro''' with Gmsh.
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To run the model, open '''grating2D.pro''' with Gmsh.
  
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This model applies to so-called mono-dimensional grating, i.e. structures having one direction of invariance. Various geometries and materials can be handled. The two classical polarization cases, denoted here E// and H//, are addressed. The output consists in a full energy balance of the problem computed from the field maps. For more detailed information and associated bibliography, the curious reader is invited refer to <ref name=Demesy2007 />.
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== References ==
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<references>
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<ref name=Demesy2007>  G. Demésy, F. Zolla, A. Nicolet, M. Commandré, and C. Fossati, [https://doi.org/10.1364/OE.15.018089 The finite element method as applied to the diffraction by an anisotropic grating], Opt. Express 15, 18089-18102 (2007).</ref>
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</references>
  
 
{{metamodelfooter|diffraction_grating}}
 
{{metamodelfooter|diffraction_grating}}

Latest revision as of 21:19, 7 July 2017

Parametric model of diffraction gratings

Download model archive (diffraction_grating.zip)
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Additional information

To run the model, open grating2D.pro with Gmsh.

This model applies to so-called mono-dimensional grating, i.e. structures having one direction of invariance. Various geometries and materials can be handled. The two classical polarization cases, denoted here E// and H//, are addressed. The output consists in a full energy balance of the problem computed from the field maps. For more detailed information and associated bibliography, the curious reader is invited refer to [1].

References

  1. G. Demésy, F. Zolla, A. Nicolet, M. Commandré, and C. Fossati, The finite element method as applied to the diffraction by an anisotropic grating, Opt. Express 15, 18089-18102 (2007).

Models developed by G. Demésy.