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11: 17.7 Special Cases of Higher ϕ s r Functions
where e f = a b c q . … where λ = c ( a b / q ) 1 2 . …
17.7.10 ϕ 7 8 ( c , q ( c ) 1 2 , q ( c ) 1 2 , a , q / a , c , d , q / d ( c ) 1 2 , ( c ) 1 2 , c q / a , a c , q , c q / d , c d ; q , c ) = ( c , c q ; q ) ( a c d , a c q / d , c d q / a , c q 2 / ( a d ) ; q 2 ) ( c d , c q / d , a c , c q / a ; q ) .
where a 2 q = b c d e q n . … where q a 2 = b c d e f . …
12: 1.4 Calculus of One Variable
And f ( x ) is continuous at c when both (1.4.1) and (1.4.3) apply. … A removable singularity of f ( x ) at x = c occurs when f ( c + ) = f ( c ) but f ( c ) is undefined. … A simple discontinuity of f ( x ) at x = c occurs when f ( c + ) and f ( c ) exist, but f ( c + ) f ( c ) . … c and d constants. …
13: 18 Orthogonal Polynomials
14: 15.13 Zeros
Let N ( a , b , c ) denote the number of zeros of F ( a , b ; c ; z ) in the sector | ph ( 1 z ) | < π . If a , b , c are real, a , b , c , c a , c b 0 , 1 , 2 , , and, without loss of generality, b a , c a + b (compare (15.8.1)), then
15.13.1 N ( a , b , c ) = { 0 , a > 0 , a + 1 2 ( 1 + S ) , a < 0 , c a > 0 , a + 1 2 ( 1 + S ) + a c + 1 S , a < 0 , c a < 0 ,
where S = sign ( Γ ( a ) Γ ( b ) Γ ( c a ) Γ ( c b ) ) . … If a , b , c , c a , or c b { 0 , 1 , 2 , } , then F ( a , b ; c ; z ) is not defined, or reduces to a polynomial, or reduces to ( 1 z ) c a b times a polynomial. …
15: Staff
  • Bille C. Carlson, Iowa State University, Chap. 19

  • Leonard C. Maximon, George Washington University, Chaps. 10, 34

  • Roderick S. C. Wong, City University of Hong Kong, Chaps. 1, 2, 18

  • Leonard C. Maximon, The George Washington University, for Chap. 34 (deceased)

  • Roderick S. C. Wong, City University of Hong Kong, for Chaps. 2, 18

  • 16: Bibliography Q
  • S.-L. Qiu and M. K. Vamanamurthy (1996) Sharp estimates for complete elliptic integrals. SIAM J. Math. Anal. 27 (3), pp. 823–834.
  • W. Qiu and R. Wong (2004) Asymptotic expansion of the Krawtchouk polynomials and their zeros. Comput. Methods Funct. Theory 4 (1), pp. 189–226.
  • C. K. Qu and R. Wong (1999) “Best possible” upper and lower bounds for the zeros of the Bessel function J ν ( x ) . Trans. Amer. Math. Soc. 351 (7), pp. 2833–2859.
  • C. Quesne (2011) Higher-Order SUSY, Exactly Solvable Potentials, and Exceptional Orthogonal Polynomials. Modern Physics Letters A 26, pp. 1843–1852.
  • 17: Bibliography C
    Bibliography C
  • B. C. Carlson and J. M. Keller (1961) Eigenvalues of Density Matrices. Phys. Rev. 121, pp. 659–661.
  • B. C. Carlson (2004) Symmetry in c, d, n of Jacobian elliptic functions. J. Math. Anal. Appl. 299 (1), pp. 242–253.
  • W. J. Cody, A. J. Strecok, and H. C. Thacher (1973) Chebyshev approximations for the psi function. Math. Comp. 27 (121), pp. 123–127.
  • CoStLy (free C-XSC library)
  • 18: 15.1 Special Notation
    19: 15.7 Continued Fractions
    t n = c + n ,
    u 2 n + 1 = ( a + n ) ( c b + n ) ,
    u 2 n = ( b + n ) ( c a + n ) .
    v n = c + n + ( b a + n + 1 ) z ,
    w n = ( b + n ) ( c a + n ) z .
    20: 28.14 Fourier Series
    The coefficients satisfy
    28.14.4 q c 2 m + 2 ( a ( ν + 2 m ) 2 ) c 2 m + q c 2 m 2 = 0 , a = λ ν ( q ) , c 2 m = c 2 m ν ( q ) ,
    28.14.7 c 2 m ν ( q ) = c 2 m ν ( q ) ,
    28.14.8 c 2 m ν ( q ) = ( 1 ) m c 2 m ν ( q ) .
    c 0 ν ( 0 ) = 1 ,