English

On the best constant for Gagliardo-Nirenberg interpolation inequalities

Analysis of PDEs 2018-01-01 v1

Abstract

In this paper we derive the best constant for the following Gagliardo-Nirenberg interpolation inequality \begin{eqnarray*} \|u\|_{L^{m+1}}\leq C_{q,m,p} \|u\|^{1-\theta}_{L^{q+1}}\|\nabla u\|^{\theta}_{L^p},\quad \theta=\frac{pd(m-q)}{(m+1)[d(p-q-1)+p(q+1)]}, \end{eqnarray*} where parameters q,m,pq,m,p respectively belong to the following two ranges: (i) p>d1p>d\geq 1, q0q\geq0 and m=m=\infty. That shows LL^{\infty}-type Gagliardo-Nirenberg interpolation inequality. (ii) p>max{1,2dd+2}p>\max\{1,\frac{2d}{d+2}\}, 0q<σ10\leq q<\sigma-1, and q<m<σq<m<\sigma, where σ\sigma is defined by σ:=(p1)d+pdp \sigma:= \frac{(p-1)d+p }{d-p} if p<dp<d; σ:=\sigma:=\infty if pdp\geq d. That gives LmL^{m}-type Gagliardo-Nirenberg interpolation inequality. The best constant Cq,m,pC_{q,m,p} is given by \begin{eqnarray*} C_{q,m,p}:=\theta^{-\frac{\theta}{p}}(1-\theta)^{\frac{\theta}{p}-\frac{1}{m+1}}M_c^{-\frac{\theta}{d}},\quad M_c:=\int_{\mathbb{R}^d}u_{c,m}^{q+1}\,dx, \end{eqnarray*} where uc,mu_{c,m} is the unique radial non-increasing solution to a generalized Lane-Emden equation. The case of equality holds when u=Auc,m(λ(xx0))u=Au_{c,m}(\lambda(x-x_0)) for any real numbers A>0A>0, λ>0\lambda >0 and x0Rdx_{0}\in \mathbb{R}^d. In particular, for the case m=+m=+\infty, the generalized Lane-Emden equation becomes a Thomas-Fermi type equation. For q=0, m=q=0,~m=\infty or d=1d=1, uc,mu_{c,m} are closed form solutions expressed in term of the incomplete Beta functions. Moreover, we show that uc,muc,u_{c,m}\to u_{c,\infty} and Cq,m,pCq,,pC_{q,m,p}\to C_{q,\infty,p} as m+m\to +\infty for d=1d=1.

Keywords

Cite

@article{arxiv.1712.10208,
  title  = {On the best constant for Gagliardo-Nirenberg interpolation inequalities},
  author = {Jian-Guo Liu and Jinhuan Wang},
  journal= {arXiv preprint arXiv:1712.10208},
  year   = {2018}
}