Flexibility above the Besson–Courtois–Gallot threshold

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

C(M):=htop(φg0) voldλ(Dg0∗M)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(Dg∗M)=1\mathrm{vol}_{d\lambda}(D_g^*M)=1

and

ℏper(Dg∗M,λcan)=ℏbar(Dg∗M,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.

References

Primary source

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

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