
Painlevk Equations and Associated Polynomials
125
tonian structure and affine Weyl symmetries of the Painlev6 equations.
Typically these polynomials arise as the "T-functions" for special so-
lutions of the Painlev6 equations and are generated through nonlinear,
three-term recurrence relations which are Toda equations that arise from
the associated Backlund transformations of the Painlev6 equations. The
coefficients of these special polynomials have some interesting, indeed
somewhat mysterious, combinatorial properties (see (Noumi M. and H.,
1998; Umemura, 1998; Umemura, 2001; Umemura, 2003)). Addition-
ally these polynomials have been expressed as special cases of Schur
polynomials, which are irreducible polynomial representations of the
general linear group
GL(n)
and arise
as
T-functions of the Kadomtsev-
Petviashvili (KP) hierarchy (Jimbo and Miwa, 1983). The Yablonskii-
Vorob'ev polynomials associated with PII are expressible in terms of
2-reduced Schur functions (Kajiwara and Masuda, 1999a; Kajiwara and
Ohta, 1996), and are related to the T-function for the rational solution
of the modified Korteweg de Vries (mKdV) equation since PII arises as a
similarity reduction of the mKdV equation. The Okamoto polynomials
associated with PIv are expressible in terms of 3-reduced Schur functions
(Kajiwara and Ohta, 1998; Noumi and Yamada, 1999) since PIv arises
as
a similarity reduction of the Boussinesq equation (cf. (Clarkson and
Kruskal, 1989)), which belongs to the so-called 3-reduction of the KP
hierarchy (Jimbo and Miwa, 1983).
It is also well-known that PII-PVI possess solutions which are express-
ible in terms of the classical special functions; these are often referred
to as "one-parameter families of solutions". For PII these special func-
tion solutions are expressed in terms of Airy functions Ai(z) (Airault,
1979; Flaschka and Newell, 1980; Gambier, 1910; Okamoto, 1986), for
PIII they are expressed in terms of Bessel functions Jv(z) (Lukashevich,
1967a; Milne et al., 1997; Murata, 1995; Okamoto, 1987c), for PIv they
are expressed in terms of Weber-Hermite (parabolic cylinder) functions
Dv(z) (Bassom et al., 1995; Gromak, 1987; Lukashevich, 196713; Mu-
rata, 1985; Okamoto, 1986), for Pv they are expressed in terms of
Whittaker functions M,,p(z), or equivalently confluent hypergeomet-
ric functions 1Fl(a; c; z) (Lukashevich, 1968; Gromak, 1976; Okamoto,
198713; Watanabe, 1995), and for PVI they are expressed in terms of
hypergeometric functions 2F1(a,
b;
c;
z)
(Fokas and Yortsos, 1981; Luka-
shevich and Yablonskii, 1967; Okamoto, 1987a); see also (Ablowitz and
Clarkson, 1991; Gromak, 197813; Gromak, 1999; Gromak and Lukashe-
vich, 1982; Tamizhmani et al., 2001). Some classical orthogonal poly-
nomials arise as particular cases of these special function solutions and
thus yield rational solutions of the associated Painlev6 equations, espe-
cially in the representation of rational solutions through determinants.