We construct infinite time blow-up solution to the following heat equation with Sobolev critical exponent and drift terms $$\begin{aligned} {\left\{ \begin{array}{ll} u_t \,=\, \Delta u\,+\,\nabla b (x) \cdot \nabla u\,+\, u^{\frac{n+2}{n-2}} ~ \text{ in } ~ \mathbb {R}^n\times (0,+\infty ),\\ u(\cdot ,0)=u_0 ~ \text{ in } ~ \mathbb {R}^n, \end{array}\right. } \end{aligned}$$where b(x) is a smooth bounded function in $$\mathbb {R}^{n}$$ with $$n\ge 5$$ and the initial datum $$u_0$$ is positive and smooth. Let $$q_j \in \mathbb {R}^n,j=1,\ldots ,k$$, be distinct nondegenerate local minimum points of b(x). Assume that an eigenvalue condition (1.6) is satisfied. We prove the existence of a positive smooth solution u(x, t) which blows up at infinite time near those points with the form $$\begin{aligned} u(x,t) \approx \sum _{j=1}^k \alpha _n \left( \frac{ \mu _j(t)}{ \mu _j(t)^2 \,+\, |x-\xi _j(t)|^2 } \right) ^{\frac{n-2}{2}}, \quad \text{ as } t\rightarrow +\infty . \end{aligned}$$Here $$\xi _j(t) \rightarrow q_j$$ and $$0<\mu _j(t)\rightarrow 0$$ exponentially as $$t\rightarrow +\infty $$.
Read full abstract