Abstract

The computational methods for the diffraction integrals that occur in the Extended Nijboer-Zernike (ENZ-) approach to circular, aberrated, defocused optical systems are reviewed and updated. In the ENZ-approach, the Debye approximation of Rayleigh’s integral for the through-focus, complex, point-spread function is evaluated in semi-analytic form. To this end, the generalized pupil function, comprising phase aberrations as well as amplitude non-uniformities, is assumed to be expanded into a series of Zernike circle polynomials, and the contribution of each of these Zernike terms to the diffraction integral is expressed in the form of a rapidly converging series (containing power functions and/or Bessel functions of various kinds). The procedure of expressing the through-focus point-spread function in terms of Zernike expansion coefficients of the pupil function can be reversed and has led to the ENZ-method of retrieval of pupil functions from measured through-focus (intensity) point-spread functions. The review and update concern the computation for systems ranging from as basic as having low NA and small defocus parameter to high-NA systems, with vector fields and polarization, meant for imaging of extended objects into a multi-layered focal region. In the period 2002-2010, the evolution of the form of the diffraction integral (DI) was dictated by the agenda of the ENZ-team in which a next instance of the DI was handled by amending the computation scheme of the previous one. This has resulted into a variety of ad hoc measures, lack of transparency of the schemes, and sometimes prohibitively slow computer codes. It is the aim of the present paper to reconstruct the whole building of computation methods, using consistently more advanced mathematical tools. These tools are ‐ explicit Zernike expansion of the focal factor in the DI, ‐ Clebsch-Gordan coefficients for the omnipresent problem of linearizing products of Zernike circle polynomials, ‐ recursions for Bessel functions, binomials and for the coefficients of algebraic functions that occur as pre-factors of the focal factor in the DI. This results in a series representation of the DI involving (spherical) Bessel functions and Clebsch-Gordan coefficients, in which the dependence of the DI on parameters of the optical configuration, on focal values, on spatial variables in the image planes, and on degree and azimuthal order of the circle polynomials are separated. This separation of dependencies, together with bounds on Clebsch-Gordan coefficients and spherical Bessel functions, facilitate the error analysis for the truncation of series, showing that in the new scheme the DI can be computed virtually without loss-of-digits. Furthermore, this separation allows for a modular implementation of the computation scheme that offers speed and flexibility when varying the various parameters and variables. The resulting scheme is pre-eminently appropriate for use in advanced optical simulations, where large defocus values, high NA and Zernike terms of high order and degree occur. [DOI: http://dx.doi.org/10.2971/jeos.2013.13044]

Highlights

  • AND OVERVIEW1.1 Nijboer-Zernike theory and its extensionThe Nijboer-Zernike (NZ-) theory of diffraction integrals was intended to produce an analytic result that, with the computational means of that time (1930–1950), led to a good approximation of the point-spread function in or close to the focal plane of a low-numerical aperture (NA), circularly symmetric, aberrated optical system

  • We have reviewed the extended Nijboer-Zernike (ENZ-)theory regarding the computation of the basic integrals over the radial pupil variable that arise from the Debye approximation of the Rayleigh diffraction integral when the generalized pupil function is expanded into Zernike circle polynomials and the integration over the azimuthal pupil variable is performed analytically

  • We have given an account of the evolution of the form of the basic ENZ-integral as occurred in the period 2002-2010, starting from the simplest case with low NA and small defocus value to the much involved case with with high NA, vector fields and polarization with an extended object being imaged into a multi-layered focal region

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Summary

Nijboer-Zernike theory and its extension

The Nijboer-Zernike (NZ-) theory of diffraction integrals was intended to produce an analytic result that, with the computational means of that time (1930–1950), led to a good approximation of the (intensity) point-spread function in or close to the focal plane of a low-NA, circularly symmetric, aberrated optical system In this theory, the wave-front aberrations are limited to a few radians, and the amplitude is assumed to be constant on the exit pupil. The development of the ENZ-approach has been continued in [17] where, based on [18], the ENZ-vector formalism is used for the computation of aerial images of extended objects This yields the same five basic diffraction integrals as in the vectorial case, except that the finite distance of the object to the entrance pupil has to be accounted for by including a magnification factor in the algebraic pre-factor of the focal factor. In [21] one can find the whole history of the optical point-spread function from the 19th century onwards, including an extensive discussion on approximation of Rayleigh’s diffraction integral by Debye’s integral

Scope and main achievements
Organization of this paper
Classical Nijboer-Zernike theory
Semi-analytic extension of the basic NZ-integral result to defocused systems
EVOLUTION OF THE FORM OF THE BASIC ENZ-INTEGRAL
COMPUTATION OF BASIC INTEGRALS
DETAILS FOR SYSTEMS WITH HIGH
10.1 Modular implementation
10.2 Computation time comparison
10.3 Assessment computational load in advanced scheme
11 CONCLUSIONS AND OUTLOOK
12 ACKNOWLEDGEMENTS
C LINEARIZATION OF PRODUCTS OF RADIAL POLYNOMIALS
G R0 -EXPANSION OF
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