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Bäcklund transformations and solution hierarchies for the third Painlevé equation
In this article our concern is with the third Painlevé equation
d2𝑦 d𝑥2 | = | 1 𝑦 | ( | d𝑦 d𝑥 | ) | 2 | – | 1 𝑥 | d𝑦 d𝑥 | + | α𝑦2 + β 𝑥 | + | γ𝑦3 | + | δ 𝑦 | , (1) |
where α, β, γ, and δ are arbitrary constants. It is well known that this equation admits a variety of types of solution and here we classify and characterize many of these. Depending on the values of the parameters the third Painlevé equation can admit solutions that may be either expressed as the ratio of two polynomials in either x or x1/3 or related to certain Bessel functions. It is thought that all exact solutions of (1) can be categorized into one or other of these hierarchies. We show how, given a few initial solutions, it is possible to use the underlying structures of these hierarchies to obtain many other solutions. In addition, we show how this knowledge concerning the continuous third Painlevé equation (1) can be adapted and used to derive exact solutions of a suitable discretized counterpart of (1). Both the continuous and discrete solutions we find are of potential importance as it is known that the third Painlevé equation has a large number of physically significant applications.
History
Publication title
Studies in Applied MathematicsVolume
98Pagination
139-194ISSN
0022-2526Department/School
School of Natural SciencesPublisher
Blackwell PublishersPlace of publication
350 Main Street, Ste 6, Malden, USA, Ma, 02148Rights statement
Copyright 1997 Massachusetts Institute of TechnologyRepository Status
- Restricted