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Recursion operator for the fully-nonlinear fifth-order equation u_t = 1 / u_{5x}^{2/3}

Determine a recursion operator for the fully-nonlinear fifth-order evolution partial differential equation u_t = 1 / u_{5x}^{2/3}. Prior analysis indicates that no standard local recursion operator of order six or less exists for this equation, and the operator is expected to be nonlocal.

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Background

The paper studies symmetry-integrable, fully-nonlinear evolution equations and maps them to known semilinear integrable equations via multipotentialisations and (generalised) hodograph transformations. While the third-order equations admit standard second-order recursion operators, the authors examine a particular fifth-order fully-nonlinear equation u_t = 1 / u_{5x}{2/3}.

In Remark 2, the authors show that this fifth-order equation does not admit a recursion operator of a commonly used local form up to sixth order, suggesting that any recursion operator for this equation must be nonlocal. Despite mapping the equation to a semilinear form with known recursion structures, the recursion operator for the original fully-nonlinear equation remains unknown.

The open problem is explicitly stated in the concluding remarks, emphasizing the need to identify a (likely nonlocal) recursion operator for the fifth-order equation to fully characterize its symmetry-integrable hierarchy.

References

It is therefore an open problem to find a recursion operator for this fully-nonlinear 5th-order equation, which we expect to be nonlocal.

From fully-nonlinear to semilinear evolution equations: two symmetry-integrable examples (2506.19070 - Euler et al., 23 Jun 2025) in Section 4, Concluding remarks