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31 Heun FunctionsProperties

§31.10 Integral Equations and Representations

Contents

§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

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

and the kernel \mathcal{K}(z,t) is a solution of the partial differential equation

31.10.3(\mathcal{D}_{z}-\mathcal{D}_{t})\mathcal{K}=0,

where \mathcal{D}_{z} is Heun’s operator in the variable z:

The contour C must be such that

where

Kernel Functions

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

where \realpart{\gamma}>0, \realpart{\delta}>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)=w_{m}(z) and W(z)=\kappa_{m}w_{m}(z), where w_{m}(z)=\mathop{(0,1)\mathit{Hf}_{{m}}\/}\nolimits\!\left(a,q_{m};\alpha,%
\beta,\gamma,\delta;z\right) and \kappa_{m} is the corresponding eigenvalue.

Example 2

Fuchs–Frobenius solutions W_{m}(z)=\tilde{\kappa}_{m}z^{{-\alpha}}\mathop{\mathit{H\!\ell}\/}\nolimits\!%
\left(1/a,q_{m};\alpha,\alpha-\gamma+1,\alpha-\beta+1,\delta;1/z\right) are represented in terms of Heun functions w_{m}(z)=\mathop{(0,1)\mathit{Hf}_{{m}}\/}\nolimits\!\left(a,q_{m};\alpha,%
\beta,\gamma,\delta;z\right) by (31.10.1) with W(z)=W_{m}(z), w(z)=w_{m}(z), and with kernel chosen from

Here \tilde{\kappa}_{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

for suitable contours C_{1}, C_{2}. The weight function is

and the kernel \mathcal{K}(z;s,t) is a solution of the partial differential equation

31.10.14\left((t-z)\mathcal{D}_{s}+(z-s)\mathcal{D}_{t}+(s-t)\mathcal{D}_{z}\right)%
\mathcal{K}=0,

where \mathcal{D}_{z} is given by (31.10.4). The contours C_{1}, C_{2} must be chosen so that

where p(t) is given by (31.10.6).

Kernel Functions

Set

31.10.17
u=\frac{(stz)^{{1/2}}}{a},
v=\left(\frac{(s-1)(t-1)(z-1)}{1-a}\right)^{{1/2}},
w=i\left(\frac{(s-a)(t-a)(z-a)}{a(1-a)}\right)^{{1/2}}.

The kernel \mathcal{K} must satisfy

This equation can be solved in terms of cylinder functions \mathop{\mathscr{C}_{{\nu}}\/}\nolimits\!\left(z\right)10.2(ii)):

where \sigma_{1} and \sigma_{2} are separation constants.

Transformation of Independent Variable

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