Download Fourier Modal Method and Its Applications in Computational by Hwi Kim PDF

By Hwi Kim

Most on hand books on computational electrodynamics are occupied with FDTD, FEM, or different particular procedure built in microwave engineering. by contrast, Fourier Modal strategy and Its purposes in Computational Nanophotonics is a whole advisor to the foundations and specified arithmetic of the updated Fourier modal approach to optical research. It takes readers during the implementation of MATLAB® codes for functional modeling of recognized and promising nanophotonic buildings. The authors additionally handle the restrictions of the Fourier modal method.

Features

  • Provides a finished consultant to the foundations, tools, and arithmetic of the Fourier modal strategy
  • Explores the rising box of computational nanophotonics
  • Presents transparent, step by step, useful factors on tips on how to use the Fourier modal approach for photonics and nanophotonics functions
  • Includes the mandatory MATLAB codes, allowing readers to build their very own code

Using this ebook, graduate scholars and researchers can know about nanophotonics simulations via a entire therapy of the math underlying the Fourier modal technique and examples of useful difficulties solved with MATLAB codes.

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Extra resources for Fourier Modal Method and Its Applications in Computational Nanophotonics

Sample text

Eigenmode. and. the. negative. Bloch. eigenmode. are. slightly. modified,. from. 19c)   j ( k x + k y + k ( g )+ ( z − z )) j ( k x + k y + k ( g )+ ( z − z )) − + The. setup. using. e x y z . and. e x y z . in. the. representation. of. positive. modes. and. negative. modes,. respectively,. is. important. because. this. is. effective. for. stabilizing. the. numerical. calculation. of. field. analysis. representation. of. the. incident. optical. field,. the. reflected. optical. field. in. the.

54c) The. total. field. distribution. E. and. H. are. obtained. in. the. respective. spatial. 15). .

N,n+m) C a,(n,n+k) (n,n+m) T = (n,n+m) Ca,(n+k+1,n+m) C(n,n+m) a,(n,n+m) (a) Ln M(n,n+m) Ln+k Ln+k+1 Ln+m U = (n,n+m) T = ... 8 Bidirectional. characterization. of. a. multiblock. for. obtaining. the. block. S-matrices:. (a). characterization. k)th. block. by. respectively. interconnection,. intuitively. between. multiple. systems,. and. are. as ( R ( n , n + m + l ) = R ( n , n + m ) + T ( n , n+ m ) I − R ( n+ m + 1 , n+ m + l ) R ( n , n + m ) ) −1 × R( n+ m+1,n+ m+l )T ( n,n+ m) . ( T ( n , n+ m + l ) = T ( n+ m + 1 , n+ m + l ) I − R ( n , n+ m ) R ( n+ m + 1 , n+ m + l ) .

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