Stieltjes polynomials are polynomial solutions of the Fuchsian equation (31.14.1). Rewrite (31.14.1) in the form
where
is a polynomial of degree not exceeding
. There exist at
most
polynomials
of degree not exceeding
such
that for
, (31.15.1) has a polynomial solution
of degree
. The
are called Van Vleck polynomials
and the corresponding
Stieltjes polynomials.
If
are the zeros of an
th degree Stieltjes polynomial
, then every zero
is either one of the parameters
or a
solution of the system of equations

If
is a zero of the Van Vleck polynomial
, corresponding to an
th degree Stieltjes polynomial
, and
are
the zeros of
(the derivative of
), then
is either a zero of
or a solution of the equation
The system (31.15.2) determines the
as the points of equilibrium
of
movable (interacting) particles with unit charges in a field of
particles with the charges
fixed at
. This is the
Stieltjes electrostatic interpretation.
The zeros
,
of the Stieltjes polynomial
are the
critical points of the function
, that is, points at which
,
, where
If the following conditions are satisfied:
and
then there are exactly
polynomials
, each of
which corresponds to each of the
ways of distributing its
zeros among
intervals
,
. In this
case the accessory parameters
are given by

If the exponent and singularity parameters satisfy (31.15.5)–(31.15.6),
then for every multi-index
, where each
is a nonnegative
integer, there is a unique Stieltjes polynomial with
zeros in the open
interval
for each
. We denote this Stieltjes
polynomial by
.
Let
and
be Stieltjes polynomials
corresponding to two distinct multi-indices
and
. The products
are mutually orthogonal over the set
:
with respect to the inner product
with weight function
The normalized system of products (31.15.8) forms an orthonormal
basis in the Hilbert space
. For further details and for the
expansions of analytic functions in this basis see Volkmer (1999).