Abstract

By a redefinition of the basis functions given in Eq. (13) of my recent paper [ J. Opt. Soc. Am. A 10, 2581 ( 1993)], the sector matrix t21(M) there can be inverted analytically.

© 1994 Optical Society of America

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References

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  1. L. Li, “Multilayer modal method for diffraction gratings of arbitrary profile, depth, and permittivity,” J. Opt. Soc. Am. A 10, 2581–2591 (1993).
    [CrossRef]
  2. L. Li, “A modal analysis of lamellar diffraction gratings in conical mountings,” J. Mod. Opt. 40, 553–573 (1993).
    [CrossRef]

1993 (2)

L. Li, “A modal analysis of lamellar diffraction gratings in conical mountings,” J. Mod. Opt. 40, 553–573 (1993).
[CrossRef]

L. Li, “Multilayer modal method for diffraction gratings of arbitrary profile, depth, and permittivity,” J. Opt. Soc. Am. A 10, 2581–2591 (1993).
[CrossRef]

Li, L.

L. Li, “Multilayer modal method for diffraction gratings of arbitrary profile, depth, and permittivity,” J. Opt. Soc. Am. A 10, 2581–2591 (1993).
[CrossRef]

L. Li, “A modal analysis of lamellar diffraction gratings in conical mountings,” J. Mod. Opt. 40, 553–573 (1993).
[CrossRef]

J. Mod. Opt. (1)

L. Li, “A modal analysis of lamellar diffraction gratings in conical mountings,” J. Mod. Opt. 40, 553–573 (1993).
[CrossRef]

J. Opt. Soc. Am. A (1)

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Equations (1)

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χ m , j ( e ) ( y ) = i τ 1 ( j ) y ω m , j ( e ) ( y ) + τ 3 ( j ) α m ω m , j ( h ) ( y ) , χ m , j ( h ) ( y ) = τ 3 ( j ) α m ω m , j ( e ) ( y ) i τ 2 ( j ) y ω m , j ( h ) ( y ) ,

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