Chern (1965) proved Heinz-type radius bounds for hypersurface graphs in Euclidean space: a graph whose mean curvature satisfies σ1≥c>0\sigma_1\ge c>0 cannot be defined over too large a ball, and — Theorem 4 of that paper — for graphs of dimension m≥3m\ge 3 with σ2≤−c<0\sigma_2\le -c<0, where σ2\sigma_2 is the second elementary symmetric function of the principal curvatures (half the scalar curvature), a radius bound R≤C(m)/cR\le C(m)/\sqrt{c} holds, but only under an auxiliary quadratic coercivity condition and with a constant that Chern himself expected to be improvable. The optimal form of this negative-scalar-curvature estimate is still unknown: the problem asks whether the bound holds under σ2≤−c\sigma_2\le -c alone, what the sharp constant is when it holds, and whether a complete entire graph in Rm+1\mathbb{R}^{m+1}, m≥3m\ge 3, can have scalar curvature bounded above by a negative constant — the graph analogue of Efimov's classical theorem, known so far only under auxiliary bounds on the second fundamental form or the mean curvature. The Gauss-map density question raised in the same 1965 paper was answered negatively by Hoffman, Osserman and Schoen (1982), whose hemisphere rigidity theorem then superseded it, so that thread is resolved and the negative-σ2\sigma_2 estimate is the sole open core.

Background

Let uu be a C2C^2 function on a domain Ω⊂Rm\Omega\subset\mathbb{R}^m. Its graph Γu={(x,u(x)):x∈Ω}\Gamma_u=\{(x,u(x)):x\in\Omega\} is a hypersurface in Rm+1\mathbb{R}^{m+1}, described at each point by the second fundamental form hijh_{ij} — the second derivatives of the immersion projected on a unit normal — or equivalently by the shape operator AA, a self-adjoint endomorphism whose eigenvalues κ1,…,κm\kappa_1,\dots,\kappa_m are the principal curvatures. The elementary symmetric functions σk=∑i1<⋯<ikκi1⋯κik\sigma_k=\sum_{i_1<\cdots<i_k}\kappa_{i_1}\cdots\kappa_{i_k} interpolate between the mean curvature (σ1\sigma_1, taken here as the sum of the principal curvatures) and the scalar curvature: by the Gauss equation the scalar curvature of the induced metric equals 2σ22\sigma_2. The Gauss map sends each point of the graph to its unit normal, a point of the unit sphere SmS^m.

A classical theme, going back to Bernstein's theorem — an entire graph in R3\mathbb{R}^3 whose mean curvature vanishes identically (a minimal graph) is a plane — is that a curvature bound limits the size of the parameter domain of a graph. Heinz (1955) proved that a surface graph over a disk of radius RR whose mean curvature is at least c>0c>0 satisfies R≤1/cR\le 1/c. Chern (1965) reorganized this circle of ideas for hypersurfaces of any dimension through integral identities for a piece of hypersurface whose normals make an angle at most aa with a fixed direction, comparing the area VaV_a of its Gauss image with the area LaL_a of its projection: when σ1≥c\sigma_1\ge c the identity reads mc Va≤Lamc\,V_a\le L_a, and when σ2≥b\sigma_2\ge b it reads m(m−1)b Va≤La\sqrt{m(m-1)b}\,V_a\le L_a. Both imply Heinz-type radius bounds for graphs, and a contemporary remark of Flanders (1966) on the mean-curvature case belongs to the same family, now usually called the Bernstein–Heinz–Chern–Flanders inequalities.

The situation changes when the curvature is bounded above by a negative constant, because the prescribed-curvature equation of the graph degenerates wherever the curvature tends to zero and no elliptic estimate applies. For surfaces, Efimov's classical theorem (Efimov 1968, in English translation) states that no complete immersed surface in R3\mathbb{R}^3 has Gauss curvature κ1κ2≤−c<0\kappa_1\kappa_2\le -c<0 everywhere. In higher dimensions the analogue is open: Smyth and Xavier (1987) settled the three-dimensional case of the extension posed independently by Reilly and Yau — a complete hypersurface in R4\mathbb{R}^4 whose Ricci curvature is bounded above by a negative constant satisfies inf⁡∥A∥=0\inf\|A\|=0, so that no such hypersurface exists — and obtained only partial results beyond dimension three. For graphs, Chern (1965, Theorem 4) proved a local analogue: a graph over a ball of radius RR in Rm\mathbb{R}^m, m≥3m\ge 3, with σ2≤−c<0\sigma_2\le -c<0, satisfies a radius bound R≤C(m)/cR\le C(m)/\sqrt{c} — but only under an auxiliary quadratic coercivity condition: a pointwise lower bound on a quadratic expression in the principal curvatures that restores control exactly where the scalar-curvature inequality degenerates. Chern remarked that the constant in this estimate can most likely be improved, and the contemporary zbMATH review of the paper likewise judged the inequality almost certainly non-sharp.

The subsequent literature has approached this estimate only through auxiliary hypotheses. Elbert (2000) proved that no complete graph with bounded ∥A∥\|A\| can have scalar curvature bounded above by a negative constant (the paper treats negative rr-th mean curvature in general); Hasanis and Vlachos (2004) obtained related rigidity for entire graphs under the same boundedness hypothesis; Fontenele (2010) proved that an entire graph with bounded mean curvature satisfies inf⁡∣R∣=0\inf|R|=0 (with RR now denoting the scalar curvature), improving results of Elbert and of Hasanis–Vlachos, and that inf⁡∥A∥=0\inf\|A\|=0 holds for entire graphs of negative Ricci curvature in dimensions n≥3n\ge 3, improving a result of Chern and giving a partial answer to a question of Smyth and Xavier; he also records Okayasu's (1989) construction of a complete O(2)×O(2)O(2)\times O(2)-invariant hypersurface of constant negative scalar curvature in R4\mathbb{R}^4 — whose unbounded ∥A∥\|A\| shows that the graph hypothesis is essential to the global question — and states explicitly that he does not know whether the bounded-mean-curvature assumption can be removed. Coswosck and Fontenele (2021) generalized and improved these estimates to graphs over complete Riemannian domains, still under Ricci-type hypotheses. On the quantitative side, Fontenele and Silva (2005) determined sharp estimates for the size of balls in the complement of a complete hypersurface with bounded ∥A∥\|A\| — a different, extrinsic setting — and Barbosa, Bessa and Montenegro (2008) extended the Bernstein–Heinz–Chern–Flanders inequalities to foliations. No known work removes Chern's coercivity condition for m≥3m\ge 3, determines the sharp constant of the σ2≤−c\sigma_2\le -c radius bound, or settles the existence of complete entire graphs with uniformly negative scalar curvature without auxiliary hypotheses.

The Gauss-map question raised in the 1965 paper is resolved. Chern (1965) raises there, on p. 83, the density question — whether the Gauss map of a complete surface with non-zero constant mean curvature is everywhere dense. Hoffman, Osserman and Schoen (1982) answered it negatively: the unduloids (complete constant-mean-curvature surfaces of revolution) have Gauss images in an arbitrarily narrow strip about a great circle, and such a strip omits open sets. The plane/cylinder rigidity is Theorem 1 of Hoffman–Osserman–Schoen (1982), under the hypothesis that the Gauss image lies in a closed hemisphere, and it was later generalized to uniformly elliptic Weingarten surfaces — surfaces whose principal curvatures satisfy a fixed elliptic relation — by Fernández, Gálvez and Mira (2023). This Gauss-map thread is resolved and contributes no open core; the open core is the negative-σ2\sigma_2 radius estimate described above.

Problem Statement

Determine the optimal Heinz-type radius estimate for hypersurface graphs with uniformly negative scalar curvature — the open core of Chern's 1965 Theorem 4. Throughout, σ2=∑i<jκiκj\sigma_2=\sum_{i<j}\kappa_i\kappa_j denotes the second elementary symmetric function of the principal curvatures of a graph in Rm+1\mathbb{R}^{m+1} with respect to the upward unit normal (equal to half the scalar curvature of the induced metric), and m≥3m\ge 3. For m=2m=2, where σ2\sigma_2 is the Gauss curvature, the coercivity-free bound is classical — Heinz's estimate inf⁡∣σ2∣≤3e2/R2\inf|\sigma_2|\le 3e^2/R^2 (with ee Euler's number) for a graph over a disk of radius RR yields R≤e3/cR\le e\sqrt{3/c} — which is why the problem below concerns m≥3m\ge 3.

(1) Coercivity-free local bound. Prove or disprove: there exists a constant C(m)C(m), depending only on mm, such that for every c>0c>0 and every C2C^2 function uu on the closed ball B‾R(0)⊂Rm\overline{B}_R(0)\subset\mathbb{R}^m whose graph has σ2≤−c\sigma_2\le -c at every point, one has R≤C(m)/cR\le C(m)/\sqrt{c}. Chern proved this only under an additional quadratic coercivity condition on the principal curvatures; the statement above imposes no coercivity, boundedness, or curvature-growth condition.

(2) Sharp constant. To the extent the bound in (1) holds, determine the optimal value of C(m)C(m): prove the bound for that value and exhibit a family of graphs over balls of radii tending to C(m)/cC(m)/\sqrt{c} from below, all with σ2≤−c\sigma_2\le -c, showing that no smaller constant is possible. An explicit constant strictly smaller than Chern's, even under a weakened coercivity condition, does not determine the optimal value of C(m)C(m).

(3) Global counterpart. Settle whether there exists a complete entire graph in Rm+1\mathbb{R}^{m+1}, m≥3m\ge 3 — a C2C^2 function on all of Rm\mathbb{R}^m whose graph, with its induced metric, is complete — with σ2≤−c<0\sigma_2\le -c<0 everywhere for some c>0c>0.

These three components share one scientific objective: the optimal local-to-global control of the parameter domain of a hypersurface graph under a uniformly negative scalar-curvature bound. They determine one another: a proof in (1) implies nonexistence in (3), because a complete entire graph restricts to graphs over balls of every radius; conversely, an affirmative construction in (3), or a sequence of graphs over balls of arbitrarily large radius with σ2≤−c\sigma_2\le -c for fixed cc, refutes (1) and shows that no finite constant exists in (2).

References

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