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Movable algebraic singularities of second-order ordinary differential equations

Any nonlinear equation of the form y ″ = ∑ n = 0 N a n ( z ) y n has a solution with leading behavior proportional to ( z − z 0 ) − 2 / ( N − 1 ) about a point z 0 , where the coefficients a n are analytic at z 0 and a N ( z 0 ) ≠ 0 . Equations are considered for which each possible leading term of...

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Bibliographic Details
Published in:Journal of mathematical physics 2009-02, Vol.50 (2), p.023509-023509-18
Main Authors: Filipuk, G., Halburd, R. G.
Format: Article
Language:English
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Summary:Any nonlinear equation of the form y ″ = ∑ n = 0 N a n ( z ) y n has a solution with leading behavior proportional to ( z − z 0 ) − 2 / ( N − 1 ) about a point z 0 , where the coefficients a n are analytic at z 0 and a N ( z 0 ) ≠ 0 . Equations are considered for which each possible leading term of this form extends to a Laurent series solution in fractional powers of z − z 0 . For these equations we show that the only movable singularities that can be reached by analytic continuation along finite-length curves are of the algebraic type just described. This generalizes results of Shimomura [“On second order nonlinear differential equations with the quasi-Painlevé property II,” RIMS Kokyuroku 1424, 177 (2005)]. The possibility that these algebraic singularities could accumulate along infinitely long paths ending at a finite point is considered. Smith [“On the singularities in the complex plane of the solutions of y ″ + y ′ f ( y ) + g ( y ) = P ( x ) ,” Proc. Lond. Math. Soc. 3, 498 (1953)] showed that such singularities do occur in solutions of a simple equation outside this class.
ISSN:0022-2488
1089-7658
DOI:10.1063/1.3068414