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11: Bibliography T
  • S. A. Teukolsky (1972) Rotating black holes: Separable wave equations for gravitational and electromagnetic perturbations. Phys. Rev. Lett. 29 (16), pp. 1114–1118.
  • E. C. Titchmarsh (1946) Eigenfunction Expansions Associated with Second-Order Differential Equations. Clarendon Press, Oxford.
  • E. C. Titchmarsh (1958) Eigenfunction Expansions Associated with Second Order Differential Equations, Part 2, Partial Differential Equations. Clarendon Press, Oxford.
  • C. A. Tracy and H. Widom (1994) Level-spacing distributions and the Airy kernel. Comm. Math. Phys. 159 (1), pp. 151–174.
  • J. F. Traub (1964) Iterative Methods for the Solution of Equations. Prentice-Hall Series in Automatic Computation, Prentice-Hall Inc., Englewood Cliffs, N.J..
  • 12: 20.13 Physical Applications
    The functions θ j ( z | τ ) , j = 1 , 2 , 3 , 4 , provide periodic solutions of the partial differential equation …with κ = i π / 4 . … Theta-function solutions to the heat diffusion equation with simple boundary conditions are discussed in Lawden (1989, pp. 1–3), and with more general boundary conditions in Körner (1989, pp. 274–281). In the singular limit τ 0 + , the functions θ j ( z | τ ) , j = 1 , 2 , 3 , 4 , become integral kernels of Feynman path integrals (distribution-valued Green’s functions); see Schulman (1981, pp. 194–195). This allows analytic time propagation of quantum wave-packets in a box, or on a ring, as closed-form solutions of the time-dependent Schrödinger equation.
    13: 12.16 Mathematical Applications
    PCFs are used as basic approximating functions in the theory of contour integrals with a coalescing saddle point and an algebraic singularity, and in the theory of differential equations with two coalescing turning points; see §§2.4(vi) and 2.8(vi). … PCFs are also used in integral transforms with respect to the parameter, and inversion formulas exist for kernels containing PCFs. …
    14: 10.73 Physical Applications
    §10.73(ii) Spherical Bessel Functions
    The analysis of the current distribution in circular conductors leads to the Kelvin functions ber x , bei x , ker x , and kei x . …
    15: Bibliography J
  • A. J. Jerri (1982) A note on sampling expansion for a transform with parabolic cylinder kernel. Inform. Sci. 26 (2), pp. 155–158.
  • M. Jimbo and T. Miwa (1981) Monodromy preserving deformation of linear ordinary differential equations with rational coefficients. II. Phys. D 2 (3), pp. 407–448.
  • D. S. Jones, M. J. Plank, and B. D. Sleeman (2010) Differential equations and mathematical biology. Chapman & Hall/CRC Mathematical and Computational Biology Series, CRC Press, Boca Raton, FL.
  • D. S. Jones and B. D. Sleeman (2003) Differential equations and mathematical biology. Chapman & Hall/CRC Mathematical Biology and Medicine Series, Chapman & Hall/CRC, Boca Raton, FL.
  • N. Joshi and A. V. Kitaev (2001) On Boutroux’s tritronquée solutions of the first Painlevé equation. Stud. Appl. Math. 107 (3), pp. 253–291.
  • 16: 18.12 Generating Functions
    18.12.2 𝐅 1 0 ( α + 1 ; ( x 1 ) z 2 ) 𝐅 1 0 ( β + 1 ; ( x + 1 ) z 2 ) = ( 1 2 ( 1 x ) z ) 1 2 α J α ( 2 ( 1 x ) z ) ( 1 2 ( 1 + x ) z ) 1 2 β I β ( 2 ( 1 + x ) z ) = n = 0 P n ( α , β ) ( x ) Γ ( n + α + 1 ) Γ ( n + β + 1 ) z n ,
    18.12.2_5 F 1 2 ( γ , α + β + 1 γ α + 1 ; 1 R z 2 ) F 1 2 ( γ , α + β + 1 γ β + 1 ; 1 R + z 2 ) = n = 0 ( γ ) n ( α + β + 1 γ ) n ( α + 1 ) n ( β + 1 ) n P n ( α , β ) ( x ) z n , R = 1 2 x z + z 2 , | z | < 1 ,
    18.12.3_5 1 + z ( 1 2 x z + z 2 ) β + 3 2 = n = 0 ( 2 β + 2 ) n ( β + 1 ) n P n ( β + 1 , β ) ( x ) z n , | z | < 1 ,
    18.12.17 1 + 2 x z + 4 z 2 ( 1 + 4 z 2 ) 3 2 exp ( 4 x 2 z 2 1 + 4 z 2 ) = n = 0 H n ( x ) n / 2 ! z n , | z | < 1 .
    See §18.18(vii) for Poisson kernels; these are special cases of bilateral generating functions.
    17: 10.1 Special Notation
    The main functions treated in this chapter are the Bessel functions J ν ( z ) , Y ν ( z ) ; Hankel functions H ν ( 1 ) ( z ) , H ν ( 2 ) ( z ) ; modified Bessel functions I ν ( z ) , K ν ( z ) ; spherical Bessel functions 𝗃 n ( z ) , 𝗒 n ( z ) , 𝗁 n ( 1 ) ( z ) , 𝗁 n ( 2 ) ( z ) ; modified spherical Bessel functions 𝗂 n ( 1 ) ( z ) , 𝗂 n ( 2 ) ( z ) , 𝗄 n ( z ) ; Kelvin functions ber ν ( x ) , bei ν ( x ) , ker ν ( x ) , kei ν ( x ) . … For older notations see British Association for the Advancement of Science (1937, pp. xix–xx) and Watson (1944, Chapters 1–3).
    18: Bibliography S
  • T. Shiota (1986) Characterization of Jacobian varieties in terms of soliton equations. Invent. Math. 83 (2), pp. 333–382.
  • B. D. Sleeman (1969) Non-linear integral equations for Heun functions. Proc. Edinburgh Math. Soc. (2) 16, pp. 281–289.
  • K. Soni (1980) Exact error terms in the asymptotic expansion of a class of integral transforms. I. Oscillatory kernels. SIAM J. Math. Anal. 11 (5), pp. 828–841.
  • R. Spigler and M. Vianello (1997) A Survey on the Liouville-Green (WKB) Approximation for Linear Difference Equations of the Second Order. In Advances in Difference Equations (Veszprém, 1995), S. Elaydi, I. Győri, and G. Ladas (Eds.), pp. 567–577.
  • R. Spigler (1984) The linear differential equation whose solutions are the products of solutions of two given differential equations. J. Math. Anal. Appl. 98 (1), pp. 130–147.
  • 19: Bibliography M
  • R. S. Maier (2005) On reducing the Heun equation to the hypergeometric equation. J. Differential Equations 213 (1), pp. 171–203.
  • R. S. Maier (2007) The 192 solutions of the Heun equation. Math. Comp. 76 (258), pp. 811–843.
  • M. Mazzocco (2001a) Rational solutions of the Painlevé VI equation. J. Phys. A 34 (11), pp. 2281–2294.
  • M. Mazzocco (2001b) Picard and Chazy solutions to the Painlevé VI equation. Math. Ann. 321 (1), pp. 157–195.
  • M. E. Muldoon (1970) Singular integrals whose kernels involve certain Sturm-Liouville functions. I. J. Math. Mech. 19 (10), pp. 855–873.
  • 20: 1.18 Linear Second Order Differential Operators and Eigenfunction Expansions
    where the integral kernel is given by …Equation (1.18.19) is often called the completeness relation. …
    Hermite’s Differential Equation, X = ( , )
    Applying equations (1.18.29) and (1.18.30), the complete set of normalized eigenfunctions being … See §18.39 for discussion of Schrödinger equations and operators. …