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21: 31.18 Methods of Computation
Independent solutions of (31.2.1) can be computed in the neighborhoods of singularities from their Fuchs–Frobenius expansions (§31.3), and elsewhere by numerical integration of (31.2.1). …The computation of the accessory parameter for the Heun functions is carried out via the continued-fraction equations (31.4.2) and (31.11.13) in the same way as for the Mathieu, Lamé, and spheroidal wave functions in Chapters 2830.
22: 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. …
23: 10.2 Definitions
§10.2(i) Bessel’s Equation
10.2.1 z 2 d 2 w d z 2 + z d w d z + ( z 2 ν 2 ) w = 0 .
This differential equation has a regular singularity at z = 0 with indices ± ν , and an irregular singularity at z = of rank 1 ; compare §§2.7(i) and 2.7(ii). …
10.2.2 J ν ( z ) = ( 1 2 z ) ν k = 0 ( 1 ) k ( 1 4 z 2 ) k k ! Γ ( ν + k + 1 ) .
10.2.3 Y ν ( z ) = J ν ( z ) cos ( ν π ) J ν ( z ) sin ( ν π ) .
24: 15.10 Hypergeometric Differential Equation
It has regular singularities at z = 0 , 1 , , with corresponding exponent pairs { 0 , 1 c } , { 0 , c a b } , { a , b } , respectively. …They are also numerically satisfactory (§2.7(iv)) in the neighborhood of the corresponding singularity.
Singularity z = 0
Singularity z = 1
Singularity z =
25: 36.6 Scaling Relations
Indices for k -Scaling of Magnitude of Ψ K or Ψ ( U ) (Singularity Index)
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
26: 31.3 Basic Solutions
31.3.2 a γ c 1 q c 0 = 0 ,
In general, one of them has a logarithmic singularity at z = 0 .
§31.3(ii) Fuchs–Frobenius Solutions at Other Singularities
Solutions (31.3.1) and (31.3.5)–(31.3.11) comprise a set of 8 local solutions of (31.2.1): 2 per singular point. …
27: 13.2 Definitions and Basic Properties
Kummer’s Equation
This equation has a regular singularity at the origin with indices 0 and 1 b , and an irregular singularity at infinity of rank one. …In effect, the regular singularities of the hypergeometric differential equation at b and coalesce into an irregular singularity at . …
13.2.11 U ( a , n , z ) = z n + 1 U ( a + n + 1 , n + 2 , z ) .
28: Bibliography M
  • E. L. Mansfield and H. N. Webster (1998) On one-parameter families of Painlevé III. Stud. Appl. Math. 101 (3), pp. 321–341.
  • O. I. Marichev (1984) On the Representation of Meijer’s G -Function in the Vicinity of Singular Unity. In Complex Analysis and Applications ’81 (Varna, 1981), pp. 383–398.
  • G. F. Miller (1966) On the convergence of the Chebyshev series for functions possessing a singularity in the range of representation. SIAM J. Numer. Anal. 3 (3), pp. 390–409.
  • M. E. Muldoon (1970) Singular integrals whose kernels involve certain Sturm-Liouville functions. I. J. Math. Mech. 19 (10), pp. 855–873.
  • B. T. M. Murphy and A. D. Wood (1997) Hyperasymptotic solutions of second-order ordinary differential equations with a singularity of arbitrary integer rank. Methods Appl. Anal. 4 (3), pp. 250–260.
  • 29: 16.21 Differential Equation
    16.21.1 ( ( 1 ) p m n z ( ϑ a 1 + 1 ) ( ϑ a p + 1 ) ( ϑ b 1 ) ( ϑ b q ) ) w = 0 ,
    With the classification of §16.8(i), when p < q the only singularities of (16.21.1) are a regular singularity at z = 0 and an irregular singularity at z = . When p = q the only singularities of (16.21.1) are regular singularities at z = 0 , ( 1 ) p m n , and . …
    30: 31.9 Orthogonality
    31.9.2 ζ ( 1 + , 0 + , 1 , 0 ) t γ 1 ( 1 t ) δ 1 ( t a ) ϵ 1 w m ( t ) w k ( t ) d t = δ m , k θ m .
    31.9.3 θ m = ( 1 e 2 π i γ ) ( 1 e 2 π i δ ) ζ γ ( 1 ζ ) δ ( ζ a ) ϵ f 0 ( q , ζ ) f 1 ( q , ζ ) q 𝒲 { f 0 ( q , ζ ) , f 1 ( q , ζ ) } | q = q m ,
    31.9.6 ρ ( s , t ) = ( s t ) ( s t ) γ 1 ( ( s 1 ) ( t 1 ) ) δ 1 ( ( s a ) ( t a ) ) ϵ 1 ,
    and the integration paths 1 , 2 are Pochhammer double-loop contours encircling distinct pairs of singularities { 0 , 1 } , { 0 , a } , { 1 , a } . …