Half Strong Ill-Posedness of $2\frac{1}{2}$D Electron Magnetohydrodynamics with Fractional Resistivity

We study the $2\frac{1}{2}$D electron magnetohydrodynamics (MHD): the electron MHD system that has $3$D magnetic field but is independent of $z$-variable. We establish a “half” strong ill-posedness result in $2\frac{1}{2}$D electron MHD with fractional resistivity $(-\mathrm{\Delta }{)}^{\alpha }$ in the supercritical Sobolev space $H^{\beta }\times H^{\beta -1}$ for $3<\beta <4-2\alpha$. Specifically, we construct small initial data $(a_0,b_0)$ whose solution develops a norm inflation in $a$ but the norm of $b$ remains small.