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    A regularity theory for parabolic equations with anisotropic non-local operators in Lq(Lp)L_{q}(L_{p}) spaces

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    In this paper, we present an Lq(Lp)L_q(L_p)-regularity theory for parabolic equations of the form: βˆ‚tu(t,x)=Laβƒ—,bβƒ—(t)u(t,x)+f(t,x),u(0,x)=0. \partial_t u(t,x)=\mathcal{L}^{\vec{a},\vec{b}}(t)u(t,x)+f(t,x),\quad u(0,x)=0. Here, Laβƒ—,bβƒ—(t)\mathcal{L}^{\vec{a},\vec{b}}(t) represents anisotropic non-local operators encompassing the singular anisotropic fractional Laplacian with measurable coefficients: Laβƒ—,0βƒ—(t)u(x)=βˆ‘i=1d∫R(u(x1,…,xiβˆ’1,xi+yi,xi+1,…,xd)βˆ’u(x))ai(t,yi)∣yi∣1+Ξ±idyi. \mathcal{L}^{\vec{a},\vec{0}}(t)u(x)=\sum_{i=1}^{d} \int_{\mathbb{R}}\left( u(x^{1},\dots,x^{i-1},x^{i}+y^{i},x^{i+1},\dots,x^{d}) - u(x) \right) \frac{a_{i}(t,y^{i})}{|y^{i}|^{1+\alpha_{i}}} \mathrm{d}y^{i} . To address the anisotropy of the operator, we employ a probabilistic representation of the solution and Calder\'on-Zygmund theory. As applications of our results, we demonstrate the solvability of elliptic equations with anisotropic non-local operators and parabolic equations with isotropic non-local operators
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