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11: 31.11 Expansions in Series of Hypergeometric Functions
Then the Fuchs–Frobenius solution at belonging to the exponent α has the expansion (31.11.1) with … For example, consider the Heun function which is analytic at z = a and has exponent α at . … Here one of the following four pairs of conditions is satisfied: …
12: 3.5 Quadrature
In the case of Chebyshev weight functions w ( x ) = ( 1 x ) α ( 1 + x ) β on [ 1 , 1 ] , with | α | = | β | = 1 2 , the nodes x k , weights w k , and error constant γ n , are as follows: … The pair
13: 28.2 Definitions and Basic Properties
This equation has regular singularities at 0 and 1, both with exponents 0 and 1 2 , and an irregular singular point at . … (28.2.1) possesses a fundamental pair of solutions w I ( z ; a , q ) , w II ( z ; a , q ) called basic solutions with …
§28.2(iii) Floquet’s Theorem and the Characteristic Exponents
28.2.16 cos ( π ν ) = w I ( π ; a , q ) = w I ( π ; a , q ) .
Either ν ^ or ν is called a characteristic exponent of (28.2.1). …
14: 27.3 Multiplicative Properties
27.3.2 f ( n ) = r = 1 ν ( n ) f ( p r a r ) .
27.3.5 d ( n ) = r = 1 ν ( n ) ( 1 + a r ) ,
27.3.6 σ α ( n ) = r = 1 ν ( n ) p r α ( 1 + a r ) 1 p r α 1 , α 0 .
27.3.10 f ( n ) = r = 1 ν ( n ) ( f ( p r ) ) a r .
15: 20 Theta Functions
Chapter 20 Theta Functions
16: 17.12 Bailey Pairs
§17.12 Bailey Pairs
Bailey Pairs
When (17.12.5) is iterated the resulting infinite sequence of Bailey pairs is called a Bailey Chain. … The Bailey pair that implies the Rogers–Ramanujan identities §17.2(vi) is: … The Bailey pair and Bailey chain concepts have been extended considerably. …
17: 36.6 Scaling Relations
Table 36.6.1: Special cases of scaling exponents for cuspoids.
singularity K β K γ 1 K γ 2 K γ 3 K γ K
For the results in this section and more extensive lists of exponents see Berry (1977) and Varčenko (1976).
18: 28.17 Stability as x ±
§28.17 Stability as x ±
If all solutions of (28.2.1) are bounded when x ± along the real axis, then the corresponding pair of parameters ( a , q ) is called stable. All other pairs are unstable. For example, positive real values of a with q = 0 comprise stable pairs, as do values of a and q that correspond to real, but noninteger, values of ν . However, if ν 0 , then ( a , q ) always comprises an unstable pair. …
19: 10.75 Tables
  • Achenbach (1986) tabulates J 0 ( x ) , J 1 ( x ) , Y 0 ( x ) , Y 1 ( x ) , x = 0 ( .1 ) 8 , 20D or 18–20S.

  • Kerimov and Skorokhodov (1985a) tabulates 5 (nonreal) complex conjugate pairs of zeros of the principal branches of Y n ( z ) and Y n ( z ) for n = 0 ( 1 ) 5 , 8D.

  • Bickley et al. (1952) tabulates x n I n ( x ) or e x I n ( x ) , x n K n ( x ) or e x K n ( x ) , n = 2 ( 1 ) 20 , x = 0 (.01 or .1) 10(.1) 20, 8S; I n ( x ) , K n ( x ) , n = 0 ( 1 ) 20 , x = 0 or 0.1 ( .1 ) 20 , 10S.

  • Kerimov and Skorokhodov (1984b) tabulates all zeros of the principal values of K n ( z ) and K n ( z ) , for n = 2 ( 1 ) 20 , 9S.

  • Zhang and Jin (1996, p. 322) tabulates ber x , ber x , bei x , bei x , ker x , ker x , kei x , kei x , x = 0 ( 1 ) 20 , 7S.

  • 20: Bibliography B
  • G. Backenstoss (1970) Pionic atoms. Annual Review of Nuclear and Particle Science 20, pp. 467–508.
  • K. L. Bell and N. S. Scott (1980) Coulomb functions (negative energies). Comput. Phys. Comm. 20 (3), pp. 447–458.
  • M. V. Berry (1977) Focusing and twinkling: Critical exponents from catastrophes in non-Gaussian random short waves. J. Phys. A 10 (12), pp. 2061–2081.
  • W. G. Bickley (1935) Some solutions of the problem of forced convection. Philos. Mag. Series 7 20, pp. 322–343.
  • W. Bühring (1994) The double confluent Heun equation: Characteristic exponent and connection formulae. Methods Appl. Anal. 1 (3), pp. 348–370.