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31 Heun FunctionsProperties

§31.10 Integral Equations and Representations

Contents
  1. §31.10(i) Type I
  2. §31.10(ii) Type II

§31.10(i) Type I

If w⁡(z) is a solution of Heun’s equation, then another solution W⁡(z) (possibly a multiple of w⁡(z)) can be represented as

31.10.1 W⁡(z)=∫C𝒦⁡(z,t)⁢w⁡(t)⁢ρ⁡(t)⁢dt

for a suitable contour C. The weight function is given by

31.10.2 ρ⁡(t)=tγ−1⁢(t−1)δ−1⁢(t−a)ϵ−1,

and the kernel 𝒦⁡(z,t) is a solution of the partial differential equation

31.10.3 (𝒟z−𝒟t)⁢𝒦=0,

where 𝒟z is Heun’s operator in the variable z:

31.10.4 𝒟z=z⁢(z−1)⁢(z−a)⁢(∂2/∂z2)+(γ⁢(z−1)⁢(z−a)+δ⁢z⁢(z−a)+ϵ⁢z⁢(z−1))⁢(∂/∂z)+α⁢β⁢z.

The contour C must be such that

31.10.5 p⁡(t)⁢(∂𝒦∂t⁢w⁡(t)−𝒦⁢dw⁡(t)dt)|C=0,

where

31.10.6 p⁡(t)=tγ⁢(t−1)δ⁢(t−a)ϵ.

Kernel Functions

Set

31.10.7 cos⁡θ =(z⁢ta)1/2,
sin⁡θ⁢cos⁡ϕ =i⁢((z−a)⁢(t−a)a⁢(1−a))1/2,
sin⁡θ⁢sin⁡ϕ =((z−1)⁢(t−1)1−a)1/2.

The kernel 𝒦 must satisfy

31.10.8 sin2⁡θ⁢(∂2𝒦∂θ2+((1−2⁢γ)⁢tan⁡θ+2⁢(δ+ϵ−12)⁢cot⁡θ)⁢∂𝒦∂θ−4⁢α⁢β⁢𝒦)+∂2𝒦∂ϕ2+((1−2⁢δ)⁢cot⁡ϕ−(1−2⁢ϵ)⁢tan⁡ϕ)⁢∂𝒦∂ϕ=0.

The solutions of (31.10.8) are given in terms of the Riemann P-symbol (see §15.11(i)) as

where σ is a separation constant. For integral equations satisfied by the Heun polynomial 𝐻𝑝n,m⁡(z) we have σ=12−δ−j, j=0,1,…,n.

For suitable choices of the branches of the P-symbols in (31.10.9) and the contour C, we can obtain both integral equations satisfied by Heun functions, as well as the integral representations of a distinct solution of Heun’s equation in terms of a Heun function (polynomial, path-multiplicative solution).

Example 1

Let

31.10.10 𝒦⁡(z,t)=(z⁢t−a)12−δ−σ⁢F12⁡(12−δ−σ+α,12−δ−σ+βγ;z⁢ta)×F12⁡(−12+δ+σ,−12+ϵ−σδ;a⁢(z−1)⁢(t−1)(a−1)⁢(z⁢t−a)),

where ℜ⁡γ>0, ℜ⁡δ>0, and C be the Pochhammer double-loop contour about 0 and 1 (as in §31.9(i)). Then the integral equation (31.10.1) is satisfied by w⁡(z)=wm⁡(z) and W⁡(z)=κm⁢wm⁡(z), where wm⁡(z)=(0,1)⁢𝐻𝑓m⁡(a,qm;α,β,γ,δ;z) and κm is the corresponding eigenvalue.

Example 2

Fuchs–Frobenius solutions Wm⁡(z)=κ~m⁢z−α⁢H⁢ℓ⁡(1/a,qm;α,α−γ+1,α−β+1,δ;1/z) are represented in terms of Heun functions wm⁡(z)=(0,1)⁢𝐻𝑓m⁡(a,qm;α,β,γ,δ;z) by (31.10.1) with W⁡(z)=Wm⁡(z), w⁡(z)=wm⁡(z), and with kernel chosen from

Here κ~m is a normalization constant and C is the contour of Example 1.

§31.10(ii) Type II

If w⁢(z) is a solution of Heun’s equation, then another solution W⁡(z) (possibly a multiple of w⁢(z)) can be represented as

31.10.12 W⁡(z)=∫C1∫C2𝒦⁡(z;s,t)⁢w⁢(s)⁢w⁢(t)⁢ρ⁡(s,t)⁢ds⁢dt

for suitable contours C1, C2. The weight function is

31.10.13 ρ⁡(s,t)=(s−t)⁢(s⁢t)γ−1⁢((1−s)⁢(1−t))δ−1⁢((1−(s/a))⁢(1−(t/a)))ϵ−1,

and the kernel 𝒦⁡(z;s,t) is a solution of the partial differential equation

31.10.14 ((t−z)⁢𝒟s+(z−s)⁢𝒟t+(s−t)⁢𝒟z)⁢𝒦=0,

where 𝒟z is given by (31.10.4). The contours C1, C2 must be chosen so that

31.10.15 p⁡(t)⁢(∂𝒦∂t⁢w⁢(t)−𝒦⁢dw⁢(t)dt)|C1 =0,
and
31.10.16 p⁡(s)⁢(∂𝒦∂s⁢w⁢(s)−𝒦⁢dw⁢(s)ds)|C2 =0,

where p⁡(t) is given by (31.10.6).

Kernel Functions

Set

31.10.17 u =(s⁢t⁢z)1/2a,
v =((s−1)⁢(t−1)⁢(z−1)1−a)1/2,
w =i⁢((s−a)⁢(t−a)⁢(z−a)a⁢(1−a))1/2.

The kernel 𝒦 must satisfy

31.10.18 ∂2𝒦∂u2+∂2𝒦∂v2+∂2𝒦∂w2+2⁢γ−1u⁢∂𝒦∂u+2⁢δ−1v⁢∂𝒦∂v+2⁢ϵ−1w⁢∂𝒦∂w=0.

This equation can be solved in terms of cylinder functions 𝒞ν⁡(z) (§10.2(ii)):

31.10.19 𝒦⁡(u,v,w)=u1−γ⁢v1−δ⁢w1−ϵ⁢𝒞1−γ⁡(u⁢σ1)⁢𝒞1−δ⁡(v⁢σ2)⁢𝒞1−ϵ⁡(i⁢w⁢σ1+σ2),

where σ1 and σ2 are separation constants.

Transformation of Independent Variable

A further change of variables, to spherical coordinates,

31.10.20 u =r⁢cos⁡θ,
v =r⁢sin⁡θ⁢sin⁡ϕ,
w =r⁢sin⁡θ⁢cos⁡ϕ,

leads to the kernel equation

31.10.21 ∂2𝒦∂r2+2⁢(γ+δ+ϵ)−1r⁢∂𝒦∂r+1r2⁢∂2𝒦∂θ2+(2⁢(δ+ϵ)−1)⁢cot⁡θ−(2⁢γ−1)⁢tan⁡θr2⁢∂𝒦∂θ+1r2⁢sin2⁡θ⁢∂2𝒦∂ϕ2+(2⁢δ−1)⁢cot⁡ϕ−(2⁢ϵ−1)⁢tan⁡ϕr2⁢sin2⁡θ⁢∂𝒦∂ϕ=0.

This equation can be solved in terms of hypergeometric functions (§15.11(i)):

with

31.10.23 m2+2⁢(α+β)⁢m−σ1=0,
p2+(α+β−γ−12)⁢p−14⁢σ2=0,
a+b =2⁢(α+β+p)−1,
a⁢b =p2−p⁡(1−α−β)−14⁢σ1,
c =γ−12−2⁢(α+β+p),
a′+b′ =δ+ϵ−1,
a′⁢b′ =−14⁢σ2,

and σ1 and σ2 are separation constants.

For integral equations for special confluent Heun functions (§31.12) see Kazakov and Slavyanov (1996).