Petrunin’s question on real projective spaces

Let m2m\ge 2, let gg be a Riemannian metric on RPm\mathbb{R}\mathbb{P}^{m}, and let sys(g)\operatorname{sys}(g) denote the length of the shortest loop representing the nontrivial element of π1(RPm)\pi_{1}(\mathbb{R}\mathbb{P}^{m}). If gcang_{\mathrm{can}} is the standard metric of constant sectional curvature 11, is it true that

Volg(RPm)Volgcan(RPm)(sys(g)π)m?\operatorname{Vol}_{g}(\mathbb{R}\mathbb{P}^{m})\ge \operatorname{Vol}_{g_{\mathrm{can}}}(\mathbb{R}\mathbb{P}^{m})\left(\frac{\operatorname{sys}(g)}{\pi}\right)^{m}?

Moreover, does equality hold only when gg has constant sectional curvature, equivalently when gg is homothetic to the standard metric?

Progress summary

Solved

A new preprint reports that the first unresolved three-dimensional case is solved, extending the known two-dimensional result and making the equality case rigid.

Petrunin’s question asks for the sharp projective-systolic inequality and characterization of equality on real projective spaces. The scan records results for dimensions 22 and 33 only.

Known results

  • On RP2\mathbb{RP}^2, the canonical metric is determined up to isometry by its volume spectrum, using rigidity, Weinstein’s theorem, and equality in Pu’s inequality.

August 2026 confirmation in RP3\mathbb{RP}^3

A new arXiv preprint reports the first open case as proved: sharp systolic inequalities establish the RP3\mathbb{RP}^3 result and rigidify equality, forcing constant sectional curvature. This is a preprint-level confirmation, with no separate referee report or independent exposition found in the scan.

Current status (as of August 2026): The cases RP2\mathbb{RP}^2 and RP3\mathbb{RP}^3 are reported as settled, while no conclusion is recorded for higher dimensions.

Sources
Sources & referencesView supporting material

Primary source

arXiv

Additional references

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