2013
DOI: 10.1016/j.optcom.2012.09.051
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Solving the inverse problem of high numerical aperture focusing using vector Slepian harmonics and vector Slepian multipole fields

Abstract: A technique using vector Slepian harmonics and vector Slepian multipole fields is presented for a general treatment of the inverse problem of high numerical aperture focusing. A prescribed intensity distribution or electric field distribution in the focal volume is approximated using numerical optimization and the corresponding illuminating field at the entrance pupil is constructed. Three examples from the recent literature are chosen to illustrate the method.

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Cited by 15 publications
(6 citation statements)
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“…Numerous studies have been conducted to address this issue. For example, a method based on vector Slepian harmonics and vector Slepian multipole fields is presented for a general treatment of the inverse problem of high numerical aperture (NA) focusing to achieve the prescribed electric field distribution in the focal volume [27]. The closest electromagnetic field to a target vectorial function is obtained by using the geometric projection of the target function to the pupil space of a high NA lens [28].…”
Section: Polarization Gratingsmentioning
confidence: 99%
“…Numerous studies have been conducted to address this issue. For example, a method based on vector Slepian harmonics and vector Slepian multipole fields is presented for a general treatment of the inverse problem of high numerical aperture (NA) focusing to achieve the prescribed electric field distribution in the focal volume [27]. The closest electromagnetic field to a target vectorial function is obtained by using the geometric projection of the target function to the pupil space of a high NA lens [28].…”
Section: Polarization Gratingsmentioning
confidence: 99%
“…This can be done in manifold ways, where a truncation of the series, which would be the classical Slepian function approach discussed above in (11), is one out of these possibilities. The more general Ansatz corresponds to the scaling function approach described above in (12), where we replace D ↓ by the kernel…”
Section: Scaling Functions Wavelets Reproducing Kernels and Fredholm ...mentioning
confidence: 99%
“…The result is used as the given right-hand side for an inverse problem, where point masses are reconstructed which approximately generate the corre sponding regional gravitational potential. Examples in other application domains are [6,15,26,33].…”
Section: Introductionmentioning
confidence: 99%
“…This treatment, beyond the scalar approximation, is necessary in several areas of science, including high-resolution microscopy, [6][7][8][9] optical trapping, 10 electron acceleration, 11 optical vortex knots, 12,13 beam shaping, etc. [14][15][16][17][18][19][20][21] Nevertheless, the Richards-Wolf integral only considers perfect spherical wavefronts 4,5 and real optical systems do not generate perfect spherical wavefronts at the exit pupil, but aberrated wavefronts. A new diffraction integral has been published in Refs.…”
Section: Introductionmentioning
confidence: 99%