It is a classical Sobolev inequality that if $\phi$ is an eigenfunction of the Laplace-Beltrami operator on a $n$-dim compact Riemannian manifold $M$ with eigenvalue $\lambda$ then $$||\phi||_{L^\infty(M)}\le c(n)\lambda^{\frac{n-1}{4}}||\phi||_{L^2(M)}.$$ It is a theorem that (possibly by P.H.Berard) that of sectional curvature of $M$ is strictly negative then the above bound can be improved in terms of $\lambda$ using dynamic properties of $M$ (ergodicity of geodesic flow etc.)
I am not sure what exactly the result is (in a talk I heard that there will be a saving of logarithm of $\lambda$). Could someone please exactly describe the result? Also please provide a reference to that as I am unable to find that.