32.8 Rational Solutions32.10 Special Function Solutions

§32.9 Other Elementary Solutions

Contents

§32.9(i) Third Painlevé Equation

Elementary nonrational solutions of \mbox{P}_{{\mbox{\scriptsize III}}} are

32.9.1w(z;\mu,0,0,-\mu\kappa^{3})=\kappa z^{{1/3}},
32.9.2w(z;0,-2\kappa,0,4\kappa\mu-\lambda^{2})=z(\kappa(\mathop{\ln\/}\nolimits z)^{2}+\lambda\mathop{\ln\/}\nolimits z+\mu),
32.9.3w(z;-\nu^{2}\lambda,0,\nu^{2}(\lambda^{2}-4\kappa\mu),0)=\dfrac{z^{{\nu-1}}}{\kappa z^{{2\nu}}+\lambda z^{{\nu}}+\mu},

with \kappa, \lambda, \mu, and \nu arbitrary constants.

In the case \gamma=0 and \alpha\delta\neq 0 we assume, as in §32.2(ii), \alpha=1 and \delta=-1. Then \mbox{P}_{{\mbox{\scriptsize III}}} has algebraic solutions iff

32.9.4\beta=2n,

with n\in\Integer. These are rational solutions in \zeta=z^{{1/3}} of the form

32.9.5w(z)=\ifrac{P_{{n^{2}+1}}(\zeta)}{Q_{{n^{2}}}(\zeta)},

where P_{{n^{2}+1}}(\zeta) and Q_{{n^{2}}}(\zeta) are polynomials of degrees n^{2}+1 and n^{2}, respectively, with no common zeros. For examples and plots see Clarkson (2003a) and Milne et al. (1997). Similar results hold when \delta=0 and \beta\gamma\neq 0.

\mbox{P}_{{\mbox{\scriptsize III}}} with \beta=\delta=0 has a first integral

32.9.6z^{2}(w^{{\prime}})^{2}+2zww^{{\prime}}=(C+2\alpha zw+\gamma z^{2}w^{2})w^{2},

with C an arbitrary constant, which is solvable by quadrature. A similar result holds when \alpha=\gamma=0. \mbox{P}_{{\mbox{\scriptsize III}}} with \alpha=\beta=\gamma=\delta=0, has the general solution w(z)=Cz^{{\mu}}, with C and \mu arbitrary constants.

§32.9(ii) Fifth Painlevé Equation

Elementary nonrational solutions of \mbox{P}_{{\mbox{\scriptsize V}}} are

32.9.7w(z;\mu,-\tfrac{1}{8},-\mu\kappa^{2},0)=1+\kappa z^{{1/2}},
32.9.8w(z;0,0,\mu,-\tfrac{1}{2}\mu^{2})=\kappa\mathop{\exp\/}\nolimits\!\left(\mu z\right),

with \kappa and \mu arbitrary constants.

\mbox{P}_{{\mbox{\scriptsize V}}}, with \delta=0, has algebraic solutions if either

32.9.9\mspace{17.0mu}(\alpha,\beta,\gamma)=(\tfrac{1}{2}\mu^{2},-\tfrac{1}{8}(2n-1)^{2},-1),

or

32.9.10\mspace{5.0mu}(\alpha,\beta,\gamma)=(\tfrac{1}{8}(2n-1)^{2},-\tfrac{1}{2}\mu^{2},1),

with n\in\Integer and \mu arbitrary. These are rational solutions in \zeta=z^{{1/2}} of the form

32.9.11w(z)=\ifrac{P_{{n^{2}-n+1}}(\zeta)}{Q_{{n^{2}-n}}(\zeta)},

where P_{{n^{2}-n+1}}(\zeta) and Q_{{n^{2}-n}}(\zeta) are polynomials of degrees n^{2}-n+1 and n^{2}-n, respectively, with no common zeros.

\mbox{P}_{{\mbox{\scriptsize V}}}, with \gamma=\delta=0, has a first integral

32.9.12z^{2}(w^{{\prime}})^{2}=(w-1)^{2}(2\alpha w^{2}+Cw-2\beta),

with C an arbitrary constant, which is solvable by quadrature. For examples and plots see Clarkson (2005). \mbox{P}_{{\mbox{\scriptsize V}}}, with \alpha=\beta=0 and \gamma^{2}+2\delta=0, has solutions w(z)=C\mathop{\exp\/}\nolimits\!\left(\pm\sqrt{-2\delta}z\right), with C an arbitrary constant.

§32.9(iii) Sixth Painlevé Equation

An elementary algebraic solution of \mbox{P}_{{\mbox{\scriptsize VI}}} is

32.9.13w(z;\tfrac{1}{2}\kappa^{2},-\tfrac{1}{2}\kappa^{2},\tfrac{1}{2}\mu^{2},\tfrac{1}{2}(1-\mu^{2}))=z^{{1/2}},

with \kappa and \mu arbitrary constants.

Dubrovin and Mazzocco (2000) classifies all algebraic solutions for the special case of \mbox{P}_{{\mbox{\scriptsize VI}}} with \beta=\gamma=0, \delta=\tfrac{1}{2}. For further examples of algebraic solutions see Andreev and Kitaev (2002), Boalch (2005, 2006), Gromak et al. (2002, §48), Hitchin (2003), Masuda (2003), and Mazzocco (2001b).