Smooth solutions of u_tt - u_xx = (u_x)^2 admit stable, explicitly written blow-up profiles with logarithmic growth, and no smooth exact self-similar blow-up exists.
Singularity formation for the higher dimensional Skyrme model in the strong field limit
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abstract
This paper concerns the formation of singularities in the classical $(5+1)$-dimensional, co-rotational Skyrme model. While it is well established that blowup is excluded in $(3+1)$-dimensions, nothing appears to be known in the higher dimensional case. We prove that the model, in the so-called strong field limit, admits an explicit self-similar solution which is asymptotically stable within backwards light cones. From a technical point of view, the main obstacle to this result is the presence of derivative nonlinearities in the corresponding evolution equation. These introduce first order terms in the linearized flow which render standard techniques useless. We demonstrate how this problem can be bypassed by using structural properties of the Skyrme model.
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Blow-up of the one-dimensional wave equation with quadratic spatial derivative nonlinearity
Smooth solutions of u_tt - u_xx = (u_x)^2 admit stable, explicitly written blow-up profiles with logarithmic growth, and no smooth exact self-similar blow-up exists.