Aubin's conjecture for the Yamabe invariant

Let (M,g)(M,g) be a smooth compact Riemannian manifold of dimension n3n\geq 3. For nonzero ψH1(M)\psi\in H_1(M), define the Yamabe functional

Ig(ψ)=M(ψ2+n24(n1)Rgψ2)dvψN2,N=2nn2,I_g(\psi)=\frac{\displaystyle\int_M \left(|\nabla\psi|^2+\frac{n-2}{4(n-1)}R_g\psi^2\right)\,\mathrm{d}v}{\|\psi\|_N^2},\qquad N=\frac{2n}{n-2},

and set

μ(M,g)=infψH1(M){0}Ig(ψ).\mu(M,g)=\inf_{\psi\in H_1(M)-\{0\}}I_g(\psi).

Here RgR_g is the scalar curvature of gg, and (Sn,gcan)(S_n,g_{can}) denotes the round sphere with its canonical metric. Aubin's conjecture. If (M,g)(M,g) is not conformal to (Sn,gcan)(S_n,g_{can}), then

μ(M,g)<μ(Sn,gcan).\mu(M,g)<\mu(S_n,g_{can}).

This strict inequality is the key estimate in the solution of the Yamabe problem: it ensures that the infimum defining the Yamabe invariant is attained outside the conformal class of the round sphere. The conjecture was subsequently proved, so its status is solved.

Sources & referencesView supporting material

Primary source

Farid Madani, “The Yamabe problem with singularities”, arXiv:0804.1717 (2009).

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