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11: Errata
The spectral theory of these operators, based on Sturm-Liouville and Liouville normal forms, distribution theory, is now discussed more completely, including linear algebra, matrices, matrices as linear operators, orthonormal expansions, Stieltjes integrals/measures, generating functions. …
  • Subsection 1.16(vii)

    Several changes have been made to

    1. (i)

      make consistent use of the Fourier transform notations ( f ) , ( ϕ ) and ( u ) where f is a function of one real variable, ϕ is a test function of n variables associated with tempered distributions, and u is a tempered distribution (see (1.14.1), (1.16.29) and (1.16.35));

    2. (ii)

      introduce the partial differential operator 𝐃 in (1.16.30);

    3. (iii)

      clarify the definition (1.16.32) of the partial differential operator P ( 𝐃 ) ; and

    4. (iv)

      clarify the use of P ( 𝐃 ) and P ( 𝐱 ) in (1.16.33), (1.16.34), (1.16.36) and (1.16.37).

  • Subsection 1.16(viii)

    An entire new Subsection 1.16(viii) Fourier Transforms of Special Distributions, was contributed by Roderick Wong.

  • Chapters 8, 20, 36

    Several new equations have been added. See (8.17.24), (20.7.34), §20.11(v), (26.12.27), (36.2.28), and (36.2.29).

  • References

    Bibliographic citations were added in §§1.13(v), 10.14, 10.21(ii), 18.15(v), 18.32, 30.16(iii), 32.13(ii), and as general references in Chapters 19, 20, 22, and 23.

  • 12: 3.8 Nonlinear Equations
    For describing the distribution of complex zeros of solutions of linear homogeneous second-order differential equations by methods based on the Liouville–Green (WKB) approximation, see Segura (2013). …
    3.8.15 p ( x ) = ( x 1 ) ( x 2 ) ( x 20 )
    Consider x = 20 and j = 19 . We have p ( 20 ) = 19 ! and a 19 = 1 + 2 + + 20 = 210 . …
    3.8.16 d x d a 19 = 20 19 19 ! = ( 4.30 ) × 10 7 .
    13: Sidebar 7.SB1: Diffraction from a Straightedge
    The intensity distribution follows | ( x ) | 2 , where is the Fresnel integral (See 7.3.4). …
    14: Funding
    The NIST DLMF project has been funded, in part, by the Knowledge & Distributed Intelligence Program of the National Science Foundation. …
    15: Bibliography O
  • F. Oberhettinger (1990) Tables of Fourier Transforms and Fourier Transforms of Distributions. Springer-Verlag, Berlin.
  • A. M. Odlyzko (1987) On the distribution of spacings between zeros of the zeta function. Math. Comp. 48 (177), pp. 273–308.
  • J. Oliver (1977) An error analysis of the modified Clenshaw method for evaluating Chebyshev and Fourier series. J. Inst. Math. Appl. 20 (3), pp. 379–391.
  • K. Ono (2000) Distribution of the partition function modulo m . Ann. of Math. (2) 151 (1), pp. 293–307.
  • 16: 10.73 Physical Applications
    Laplace’s equation governs problems in heat conduction, in the distribution of potential in an electrostatic field, and in hydrodynamics in the irrotational motion of an incompressible fluid. … See Krivoshlykov (1994, Chapter 2, §2.2.10; Chapter 5, §5.2.2), Kapany and Burke (1972, Chapters 4–6; Chapter 7, §A.1), and Slater (1942, Chapter 4, §§20, 25). … The analysis of the current distribution in circular conductors leads to the Kelvin functions ber x , bei x , ker x , and kei x . …
    17: 36.5 Stokes Sets
    36.5.4 80 x 5 40 x 4 55 x 3 + 5 x 2 + 20 x 1 = 0 ,
    36.5.7 X = 9 20 + 20 u 4 Y 2 20 u 2 + 6 u 2 sign ( z ) ,
    The distribution of real and complex critical points in Figures 36.5.5 and 36.5.6 follows from consistency with Figure 36.5.1 and the fact that there are four real saddles in the inner regions. …
    18: 8 Incomplete Gamma and Related
    Functions
    19: 28 Mathieu Functions and Hill’s Equation
    20: 9.9 Zeros
    §9.9(i) Distribution and Notation
    For the distribution in of the zeros of Ai ( z ) σ Ai ( z ) , where σ is an arbitrary complex constant, see Muraveĭ (1976) and Gil and Segura (2014). …
    9.9.6 a k = T ( 3 8 π ( 4 k 1 ) ) ,
    9.9.7 Ai ( a k ) = ( 1 ) k 1 V ( 3 8 π ( 4 k 1 ) ) ,
    9.9.8 a k = U ( 3 8 π ( 4 k 3 ) ) ,