31.13 Asymptotic Approximations31.15 Stieltjes Polynomials

§31.14 General Fuchsian Equation

Contents

§31.14(i) Definitions

The general second-order Fuchsian equation with N+1 regular singularities at z=a_{j}, j=1,2,\dots,N, and at \infty, is given by

31.14.1 {\frac{{d}^{2}w}{{dz}^{2}}+\left(\sum _{{j=1}}^{N}\frac{\gamma _{j}}{z-a_{j}}\right)\frac{dw}{dz}+\left(\sum _{{j=1}}^{N}\frac{q_{j}}{z-a_{j}}\right)w=0}, \sum _{{j=1}}^{N}q_{j}=0.

The exponents at the finite singularities a_{j} are \{ 0,{1-\gamma _{j}}\} and those at \infty are \{\alpha,\beta\}, where

31.14.2
\alpha+\beta+1=\sum _{{j=1}}^{N}\gamma _{j},
\alpha\beta=\sum _{{j=1}}^{N}a_{j}q_{j}.

The three sets of parameters comprise the singularity parameters a_{j}, the exponent parameters \alpha,\beta,\gamma _{j}, and the N-2 free accessory parameters q_{j}. With a_{1}=0 and a_{2}=1 the total number of free parameters is 3N-3. Heun’s equation (31.2.1) corresponds to N=3.

§31.14(ii) Kovacic’s Algorithm

An algorithm given in Kovacic (1986) determines if a given (not necessarily Fuchsian) second-order homogeneous linear differential equation with rational coefficients has solutions expressible in finite terms (Liouvillean solutions). The algorithm returns a list of solutions if they exist.

For applications of Kovacic’s algorithm in spatio-temporal dynamics see Rod and Sleeman (1995).