Let $M$ be a complete, non-compact, simply connected Riemannian manifold of dimension $n$ whose sectional curvatures are bounded above by $\kappa<0$. I want to prove that for any open subset $\Omega\subset M$ whose closure in $M$ is compact, the following inequality holds: $$\frac{Vol(\Omega)}{Vol(\partial \Omega)}\leq \frac{1}{(n-1)\sqrt{-\kappa}}$$


The constant on the right gives a lower bound for the first Dirichlet eigenvalue of the Laplace operator. If the metric on $M$ is given by $ds^2=g\_{ij}dx^idx^j$, then $$\Delta=\frac{1}{\sqrt{\det g}}\sum\_{i,j} \frac{\partial}{\partial x^i}\left(\sqrt{\det g} g\_{ij} \frac{\partial}{\partial x^j}\right)$$ If $0<\lambda\_1<\lambda2<\cdots$ are the Dirichlet eigenvalues of $-\Delta$, by a theorem of Mckean we have an inequality $$\lambda\_1(M)\geq \frac{1}{4}(n-1)^2k$$ for a Riemannian manifold satisfying the conditions above.


Is there a way to relate the first eigenvalue to the ratio of volumes so as to prove the isoperimetric inequality above or is all this the wrong strategy?


Thanks in advance for any insight.



Isoperimetric inequality in negative sectional curvature
I do not know if there is a way to get the isoperimetric inequality from the spectral gap, but both can be proven in almost the same way. The classical references for the linear isoperimetric inequality are S.-T. Yau, "Isoperimetric constants and the first eigenvalue of a compact Riemannian manifold", *Ann. Sci. École Norm. Sup.* (4) 8 (1975), no. 4, 487–507 and
Yurii D. Burago and Victor A. Zalgaller, "Geometric inequalities".


I like this proof so let me give it here (this is Burago-Zalgaller presentation). For any unit tangent vector $u$ and positive real $r$, let $s(u,r)$ be the "candle function" defined by
$$dy = s(u,r) \,du \,dr$$
when $y=\exp\_x(ru)$ and $u\in UT\_xM$. Up to a normalization, this is simply the jacobian of the exponential map. The curvature hypothesis implies $(\log s(u,r))'\geqslant \sqrt{-\kappa}(n-1)$ where the prime denotes derivative with respect to $r$ (this is a consequence of *Günther's inequality*).


$\Omega$ is contained in the union of all geodesic rays from any fixed point $x\_0$ to $\partial \Omega$. Let $U\subset UT\_{x\_0}M$ be the set of unit vectors generating geodesics that intersect $\Omega$, and for $u\in U$ let $r\_u$ be the last intersection time of the geodesic generated by $u$ with $\Omega$. Then  

$$\mathrm{Vol}(\partial \Omega) \geqslant \int\_U s(u,r\_u) \,du$$
and
$$\mathrm{Vol}(\Omega) \leqslant \int\_U \int\_0^{r\_u} s(u,t) \,dt\,du.$$


Now, writing $s(u,r\_u)=\int\_0^{r\_u} s'(u,t) \,dt$ and using Günther's inequality, the desired result comes.


I cannot help self-advertising: in fact, the same conclusions (Günther inequality, hence both the linear isoperimetric inequality and the spectral gap of MCKean) hold under a weaker curvature bound (some higher but non-positive sectional curvature can be compensated by enough more negative sectional curvature in other directions). This is explained in an arXiv paper with Greg Kuperberg, "A refinement of Günther's candle inequality" [[arXiv:1204.3943](http://arxiv.org/abs/1204.3943)].


