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We prove explicit upper and lower bounds for the Poisson hierarchy, the averaged L1-moment spectra $\left \{\frac {\mathcal {A}_{k}\left ({B_{R}^{M}}\right )}{\text {vol}\left ({S_{R}^{M}}\right )}\right \}_{k=1}^{\infty }$ A k B R M vol S R M k = 1 ∞ , and the torsional rigidity $\mathcal {A}_{1}({B^{M}_{R}})$ A 1 ( B R M ) of a geodesic ball ${B^{M}_{R}}$ B R M in a Riemannian manifold Mn which satisfies that the mean curvatures of the geodesic spheres ${S^{M}_{r}}$ S r M included in it, (up to the boundary ${S^{M}_{R}}$ S R M ), are controlled by the radial mean curvature of the geodesic spheres $S^{\omega }_{r}(o_{\omega })$ S r ω ( o ω ) with same radius centered at the center oω of a rotationally symmetric model space $M^{n}_{\omega }$ M ω n . As a consecuence, we prove a first Dirichlet eigenvalue $\lambda _{1}({B^{M}_{R}})$ λ 1 ( B R M ) comparison theorem and show that equality with the bound $\lambda _{1}(B^{\omega }_{R}(o_{\omega }))$ λ 1 ( B R ω ( o ω ) ) , (where $B^{\omega }_{r}(o_{\omega })$ B r ω ( o ω ) is the geodesic r-ball in $M^{n}_{\omega }$ M ω n ), characterizes the L1-moment spectrum $\left \{\mathcal {A}_{k}({B^{M}_{R}})\right \}_{k=1}^{\infty }$ A k ( B R M ) k = 1 ∞ as the sequence $\left \{\mathcal {A}_{k}(B^{\omega }_{R})\right \}_{k=1}^{\infty }$ A k ( B R ω ) k = 1 ∞ and vice-versa.
We prove explicit upper and lower bounds for the Poisson hierarchy, the averaged L1-moment spectra $\left \{\frac {\mathcal {A}_{k}\left ({B_{R}^{M}}\right )}{\text {vol}\left ({S_{R}^{M}}\right )}\right \}_{k=1}^{\infty }$ A k B R M vol S R M k = 1 ∞ , and the torsional rigidity $\mathcal {A}_{1}({B^{M}_{R}})$ A 1 ( B R M ) of a geodesic ball ${B^{M}_{R}}$ B R M in a Riemannian manifold Mn which satisfies that the mean curvatures of the geodesic spheres ${S^{M}_{r}}$ S r M included in it, (up to the boundary ${S^{M}_{R}}$ S R M ), are controlled by the radial mean curvature of the geodesic spheres $S^{\omega }_{r}(o_{\omega })$ S r ω ( o ω ) with same radius centered at the center oω of a rotationally symmetric model space $M^{n}_{\omega }$ M ω n . As a consecuence, we prove a first Dirichlet eigenvalue $\lambda _{1}({B^{M}_{R}})$ λ 1 ( B R M ) comparison theorem and show that equality with the bound $\lambda _{1}(B^{\omega }_{R}(o_{\omega }))$ λ 1 ( B R ω ( o ω ) ) , (where $B^{\omega }_{r}(o_{\omega })$ B r ω ( o ω ) is the geodesic r-ball in $M^{n}_{\omega }$ M ω n ), characterizes the L1-moment spectrum $\left \{\mathcal {A}_{k}({B^{M}_{R}})\right \}_{k=1}^{\infty }$ A k ( B R M ) k = 1 ∞ as the sequence $\left \{\mathcal {A}_{k}(B^{\omega }_{R})\right \}_{k=1}^{\infty }$ A k ( B R ω ) k = 1 ∞ and vice-versa.
Given a Riemmanian manifold, we provide a new method to compute a sharp upper bound for the first eigenvalue of the Laplacian for the Dirichlet problem on a geodesic ball of radius less than the injectivity radius of the manifold. This upper bound is obtained by transforming the metric tensor into a rotationally symmetric metric tensor that preserves the area of the geodesic spheres. The provided upper bound can be computed using only the area function of the geodesic spheres contained in the geodesic ball and it is sharp in the sense that the first eigenvalue of geodesic ball coincides with our upper bound if and only if the mean curvature pointed inward of each geodesic sphere is a radial function.
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