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Optimal transport, Euler equations, Mather and DiPerna-Lions theories

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1.5. THE (ANISOTROPIC) ISOPERIMETRIC INEQUALITY 23<br />

An application to Cheeger sets<br />

A Cheeger set E for an open subset Ω ⊂ Rn , n ≥ 2, is any minimizer of the variational problem<br />

<br />

P (E)<br />

cm(Ω) := inf | E ⊂ Ω, 0 < |E| < ∞ .<br />

|E| m<br />

In order to avoid trivial situations, it is assumed that Ω has finite measure <strong>and</strong> that the parameter<br />

m satisfies the constraint<br />

n − 1<br />

m > . (1.5.9)<br />

n<br />

An interesting question is how to provide lower bounds on cm(Ω) in terms of geometric properties<br />

of Ω. The basic estimate in this direction is the Cheeger inequality,<br />

|Ω| m−(n−1)/n cm(Ω) ≥ |B| m−(n−1)/n cm(B) , (1.5.10)<br />

where B is the Euclidean unit ball. The bound is sharp, in the sense that equality holds in<br />

(1.5.10) if <strong>and</strong> only if Ω = x0 + rB for some x0 ∈ R n <strong>and</strong> r > 0. In [20] we strengthen this lower<br />

bound in terms of the Fraenkel asymmetry of Ω<br />

A(Ω) := inf<br />

x∈Rn <br />

|Ω∆Br(x)|<br />

|E|<br />

<br />

: |Br| = |E| ,<br />

Theorem 1.5.3 Let Ω be an open set in Rn , n ≥ 2, with |Ω| < ∞, <strong>and</strong> let m satisfy (1.5.9).<br />

Then<br />

|Ω| m−(n−1)/n cm(Ω) ≥ |B| m−(n−1)/n <br />

2<br />

A(Ω)<br />

cm(B) 1 +<br />

,<br />

C(n, m)<br />

where C(n, m) is a constant depending only on n <strong>and</strong> m. A possible value for C(m, n) is given<br />

by<br />

2<br />

C(n, m) =<br />

+ C0(n),<br />

m − (n − 1)/n<br />

where C0(n) is the constant defined in Theorem 1.5.1.<br />

1.5.2 An isoperimetric-type inequality on constant curvature manifolds<br />

In the case of a Riemannian manifold (M, g), one can try to mimic Gromov’s proof to obtain an<br />

isoperimetric type inequality. However in this case things become extremely more complicated,<br />

since many computations which are trivial on R n involves second derivatives of the distance, <strong>and</strong><br />

so in particular Jacobi fields. In [16], in collaboration with Yuxin Ge, we succeeded in adapting<br />

Gromov’s argument to the case of the sphere <strong>and</strong> the hyperbolic space.<br />

More precisely, let M n (K) denote the n-dimensional simply connected Riemannian manifold<br />

with constant sectional curvature K ∈ R. Set c(x, y) := 1<br />

2 dg(x, y) 2 , where dg(x, y) is the geodesic<br />

distance between x <strong>and</strong> y on M, <strong>and</strong> for K ∈ R define<br />

⎧<br />

<br />

⎪⎨<br />

GK(r) :=<br />

⎪⎩<br />

( √ Kr) cos( √ Kr)<br />

sin( √ Kr)<br />

if K > 0,<br />

1<br />

<br />

if K = 0,<br />

if K < 0,<br />

( √ |K|r) cosh( √ |K|r)<br />

sinh( √ |K|r)

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