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公开(公告)号:NL2005733A
公开(公告)日:2011-06-09
申请号:NL2005733
申请日:2010-11-22
Applicant: ASML NETHERLANDS BV
Inventor: SETIJA IRWAN , KRAAIJ MARKUS , DIRKS REMCO , BEURDEN MARTIJN CONSTANT
Abstract: Numerical calculation of electromagnetic scattering properties and structural parameters of periodic structures is disclosed. A reflection coefficient has a representation as a bilinear or sesquilinear form. Computations of reflection coefficients and their derivatives for a single outgoing direction can benefit from an adjoint-state variable. Because the linear operator is identical for all angles of incidence that contribute to the same outgoing wave direction, there exists a single adjoint-state variable that generates all reflection coefficients from all incident waves that contribute to the outgoing wave. This adjoint-state variable can be obtained by numerically solving a single linear system, whereas one otherwise would need to solve a number of linear systems equal to the number of angles of incidence.
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公开(公告)号:NL2013312A
公开(公告)日:2015-03-10
申请号:NL2013312
申请日:2014-08-08
Applicant: ASML NETHERLANDS BV
Inventor: BEURDEN MARTIJN CONSTANT
Abstract: A method of calculating electromagnetic scattering properties of a structure, the structure including materials of differing properties and the structure being periodic in at least one lateral direction and extending in a vertical direction, comprises: numerically solving a volume integral equation for electromagnetic scattering for a plurality of modes in the at least one lateral direction, by performing, for each respective mode, integration (1350) of a pseudo-spectral polynomial (Chebyshev) expansion in the vertical direction multiplied by a ID Green's function using the same sample points in the orthogonal direction for all of the plurality of modes. The integration is performed by solving a regularized linear system of equations between first (1116) and second (1120) discrete transformation steps to compute (1118) values of a regularized Chebyshev expansion coefficient vector (γ). Electromagnetic scattering properties of the structure are calculated using the results of the numerical solution.
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