Linear ill-posedness of three-dimensional MHD boundary layer equations

We prove linear ill-posedness in tangential Sobolev spaces for the three-dimensional resistive MHD boundary layer equations. We assume that a suitable linear combination of the initial tangential velocity components has a non-degenerate critical point and that both initial tangential magnetic components have a double zero at the same point. Compared with the corresponding two-dimensional MHD result, our construction requires only this double-zero condition, rather than a higher-order degeneracy of the magnetic shear. The proof combines the three-dimensional Prandtl critical layer construction with a vector correction to the two-dimensional magnetic quotient. This correction cancels the leading terms in both induction equations while preserving the magnetic divergence constraint. The resulting approximate solutions grow like $\exp (\sigma t\mathrm{/}\sqrt{\epsilon })$, and their residuals have a prefactor of order $O({\epsilon }^{-3\mathrm{/}8})$, up to logarithmic factors. A Duhamel argument then yields linear ill-posedness for every tangential derivative loss $\mu <\frac{1}{8}$. Thus the three-dimensional Prandtl instability persists when the stabilizing tangential magnetic field degenerates.