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39 39 32 10 2 61 57 44 5 1 18 16 13 8 0 40 37 24 10 4 62 59 55 5 3 19 18 18 8 2 41 38 31 10 6 63 61 68 5 5 20 20 25 8 4 42 40 40 10 8 64 63 83 6 −6 21 27 37 8 6 43 42 51 10 10 65 65 100

      It must be stated, at this point, that the 36 polynomials used, in this instance, are not those that would be ordered as in Table 5.1. That is to say, they are not the first 36 ANSI standard polynomials. As mentioned earlier, there are, unfortunately, a number of competing conventions for the numbering of Zernike polynomials. The convention used in determining the P to Vr figure is the so called Zernike Fringe polynomial convention. The logic of ordering the polynomials in a different way is that this better reflects, in the case of the fringe polynomial set, the spatial frequency content of the polynomial and its practical significance in real optical systems.

      5.3.5 Other Zernike Numbering Conventions

      1 American National Standards Institute (2017). Methods for Reporting Optical Aberrations of Eyes, ANSI Z80.28:2017. Washington DC: ANSI.

      2 Born, M. and Wolf, E. (1999). Principles of Optics, 7e. Cambridge: Cambridge University Press. ISBN: 0-521-642221.

      3 Fischer, R.E., Tadic-Galeb, B., and Yoder, P.R. (2008). Optical System Design, 2e. Bellingham: SPIE. ISBN: 978-0-8194-6785-0.

      4 Hecht, E. (2017). Optics, 5e. Harlow: Pearson Education. ISBN: 978-0-1339-7722-6.

      5 Noll, R. (1976). Zernike polynomials and atmospheric turbulence. J. Opt. Soc. Am. 66 (3): 207.

      6 Zernike, F. (1934). Beugungstheorie des Schneidenverfahrens und Seiner Verbesserten Form, der Phasenkontrastmethode. Physica 1 (8): 689.

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