Global self-similar solutions for Hardy-Hénon equations with linear and quasilinear diffusion
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| Formato: | Preprint |
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2026
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| _version_ | 1866914347066851328 |
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| author | Iagar, Razvan Gabriel Sánchez, Ariel Sarrion-Pedralva, Erik |
| author_facet | Iagar, Razvan Gabriel Sánchez, Ariel Sarrion-Pedralva, Erik |
| contents | Global self-similar solutions to the parabolic Hardy-Hénon equation $$ u_t=Δu^m+|x|^σu^p, \quad (x,t)\in\mathbb{R}^N\times(0,\infty), $$ are classified in the range of exponents $m\geq1$, $p>m$ and $σ>\max\{-2,-N\}$. The classification varies strongly with respect to the celebrated \emph{Fujita} and \emph{Sobolev critical exponents} $$ p_F(σ)=m+\frac{σ+2}{N}, \quad p_S(σ)=
\begin{cases}
\frac{m(N+2σ+2)}{N-2}, & \mbox{if } N\geq3, \\[1mm]
\infty, & \mbox{if } N\in\{1,2\}.
\end{cases} $$ Indeed, if $p\in(p_F(σ),p_S(σ))$, both equations admit self-similar solutions with either compact support (if $m>1$) or Gaussian-like tail as $|x|\to\infty$ (if $m=1$), as well as a one-parameter family satisfying $$ u(x,t)\sim C|x|^{-(σ+2)/(p-m)}, \quad {\rm as} \ |x|\to\infty. $$ If $p\geq p_S(σ)$, there are only self-similar solutions with the latter algebraic tail, while for $m<p\leq p_F(σ)$ no global solutions exist. The results open the way for a deeper study of the role of these solutions in the dynamics of the Hardy-Hénon equations. |
| format | Preprint |
| id |
arxiv_https___arxiv_org_abs_2602_20699 |
| institution | arXiv |
| publishDate | 2026 |
| record_format | arxiv |
| spellingShingle | Global self-similar solutions for Hardy-Hénon equations with linear and quasilinear diffusion Iagar, Razvan Gabriel Sánchez, Ariel Sarrion-Pedralva, Erik Analysis of PDEs Dynamical Systems Global self-similar solutions to the parabolic Hardy-Hénon equation $$ u_t=Δu^m+|x|^σu^p, \quad (x,t)\in\mathbb{R}^N\times(0,\infty), $$ are classified in the range of exponents $m\geq1$, $p>m$ and $σ>\max\{-2,-N\}$. The classification varies strongly with respect to the celebrated \emph{Fujita} and \emph{Sobolev critical exponents} $$ p_F(σ)=m+\frac{σ+2}{N}, \quad p_S(σ)= \begin{cases} \frac{m(N+2σ+2)}{N-2}, & \mbox{if } N\geq3, \\[1mm] \infty, & \mbox{if } N\in\{1,2\}. \end{cases} $$ Indeed, if $p\in(p_F(σ),p_S(σ))$, both equations admit self-similar solutions with either compact support (if $m>1$) or Gaussian-like tail as $|x|\to\infty$ (if $m=1$), as well as a one-parameter family satisfying $$ u(x,t)\sim C|x|^{-(σ+2)/(p-m)}, \quad {\rm as} \ |x|\to\infty. $$ If $p\geq p_S(σ)$, there are only self-similar solutions with the latter algebraic tail, while for $m<p\leq p_F(σ)$ no global solutions exist. The results open the way for a deeper study of the role of these solutions in the dynamics of the Hardy-Hénon equations. |
| title | Global self-similar solutions for Hardy-Hénon equations with linear and quasilinear diffusion |
| topic | Analysis of PDEs Dynamical Systems |
| url | https://arxiv.org/abs/2602.20699 |