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1: DLMF Project News
error generating summary
2: Foreword
However, we have also seen the birth of a new age of computing technology, which has not only changed how we utilize special functions, but also how we communicate technical information. …
3: Frank W. J. Olver
Having witnessed the birth of the computer age firsthand (as a colleague of Alan Turing at NPL, for example), Olver is also well known for his contributions to the development and analysis of numerical methods for computing special functions. … He continued his editing work until the time of his death on April 22, 2013 at age 88.
4: Publications
  • R. Boisvert, C. W. Clark, D. Lozier and F. Olver (2011) A Special Functions Handbook for the Digital Age, Notices of the American Mathematical Society 58, 7 (2011), pp. 905–911. PDF
  • 5: 4.3 Graphics
    See accompanying text
    Figure 4.3.1: ln x and e x . Parallel tangent lines at ( 1 , 0 ) and ( 0 , 1 ) make evident the mirror symmetry across the line y = x , demonstrating the inverse relationship between the two functions. Magnify
    6: 36.7 Zeros
    Near z = z n , and for small x and y , the modulus | Ψ ( E ) ( 𝐱 ) | has the symmetry of a lattice with a rhombohedral unit cell that has a mirror plane and an inverse threefold axis whose z and x repeat distances are given by …
    7: 19.3 Graphics
    See accompanying text
    Figure 19.3.1: K ( k ) and E ( k ) as functions of k 2 for 2 k 2 1 . Graphs of K ( k ) and E ( k ) are the mirror images in the vertical line k 2 = 1 2 . Magnify
    8: Bibliography B
  • M. V. Berry (1975) Cusped rainbows and incoherence effects in the rippling-mirror model for particle scattering from surfaces. J. Phys. A 8 (4), pp. 566–584.
  • 9: Bibliography M
  • Yu. I. Manin (1998) Sixth Painlevé Equation, Universal Elliptic Curve, and Mirror of 𝐏 2 . In Geometry of Differential Equations, A. Khovanskii, A. Varchenko, and V. Vassiliev (Eds.), Amer. Math. Soc. Transl. Ser. 2, Vol. 186, pp. 131–151.
  • 10: 18.39 Applications in the Physical Sciences
    The Schrödinger operator essential singularity, seen in the accumulation of discrete eigenvalues for the attractive Coulomb problem, is mirrored in the accumulation of jumps in the discrete Pollaczek–Stieltjes measure as x 1 . …