Abstract

We consider the focusing modified Zakharov–Kuznetsov (mZK) equation in two space dimensions. We prove that solutions which blow up in finite time in the \(H^1(\mathbb {R}^{2})\) norm have the property that they concentrate a non-trivial portion of their mass (more precisely, at least the amount equal to the mass of the ground state) at the blow-up time. For finite-time blow-up solutions in the \(H^s(\mathbb {R}^2)\) norm for \(\frac{17}{18}< s < 1\), we prove a slightly weaker result. Moreover, we prove that the stronger concentration result can be extended to the range \( \frac{17}{18} < s \le 1\) under an additional assumption on the upper bound of the blow-up rate of the solution. The main tools used here are the I-method and a profile decomposition theorem for a bounded family of \(H^1(\mathbb {R}^{2})\) functions.

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