Flexibility above the Besson–Courtois–Gallot threshold

Let MnM^n be a closed manifold admitting a negatively curved locally symmetric metric g0g_0. Define

C(M):=htop(φg0)voldλ(Dg0M)1/n.C(M):=h_{\mathrm{top}}(\varphi_{g_0})\,\mathrm{vol}_{d\lambda}(D_{g_0}^*M)^{1/n}.

Flexibility above the Besson–Courtois–Gallot threshold. For every

c>C(M),c>C(M),

there exists a negatively curved Riemannian metric gg on MM such that

voldλ(DgM)=1\mathrm{vol}_{d\lambda}(D_g^*M)=1

and

per(DgM,λcan)=bar(DgM,λcan)=c.\hbar_{\rm per}(D_g^*M,\lambda_{\mathrm{can}})=\hbar_{\rm bar}(D_g^*M,\lambda_{\mathrm{can}})=c.

This is the higher-dimensional entropy-flexibility problem above the Besson–Courtois–Gallot threshold. The supplied text does not establish the statement or indicate whether it has been resolved.

Sources & referencesView supporting material

Primary source

Wenmin Gong, “Persistent Entropy of Floer Persistence Barcodes”, arXiv:2606.19071 (2026).

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