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In this paper, we study the regularity criterion of weak solutions to the
three-dimensional (3D) MHD equations. It is proved that the solution
becomes regular provided that one velocity and one current density component of
the solution satisfy% \begin{equation} u_{3}\in L^{\frac{30\alpha }{7\alpha
-45}}\left( 0,T;L^{\alpha ,\infty }\left( ^{3}\right) \right) \text{
\ \ \ with \ \ }\frac{45}{7}% \leq \alpha \leq \infty , \label{eq01}
\end{equation}% and \begin{equation} j_{3}\in L^{\frac{2\beta }{2\beta
-3}}\left( 0,T;L^{\beta ,\infty }\left( ^{3}\right) \right) \text{
\ \ with \ \ }\frac{3}{2}\leq \beta \leq \infty , \label{eq02} \end{equation}%
which generalize some known results.

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