Gao (Math. Res. Lett. 2025) generalized Huang's Lemma — the central rigidity tool for proper holomorphic mappings between balls and hyperquadrics — by proving that solutions of ∑j=1n′φj(z)ψj(z)=∥z∥r,s2H(z,zˉ)\sum_{j=1}^{n'}\varphi_j(z)\psi_j(z)=\|z\|^2_{r,s}H(z,\bar z) with r+s≤n′≤2(r+s)−3r+s\le n'\le 2(r+s)-3 and H≢0H\not\equiv 0 have a rank-one multiplier H=h1h2H=h_1h_2 and partially linear structure, and correspondingly that local orthogonal pairs from Pr,s,tP^{r,s,t} into Pn′,0P^{n',0} are quasi-standard or null. A generalized Whitney map shows that both conclusions fail at the borderline n′=2(r+s)−2n'=2(r+s)-2, where the multiplier can have Hermitian rank greater than one, and no structural description is known there; likewise the classification of local orthogonal pairs between Pr,sP^{r,s} and indefinite targets Pr′,s′P^{r',s'} is available only in restricted ranges. The problem is to classify the local structure of orthogonal pairs (equivalently, of solutions of the generalized Huang equation) at this borderline codimension — whether every pair is null, quasi-standard, or of Whitney type — and to complete the classification for indefinite targets in the ranges not covered by existing rigidity theorems, which is exactly the input the transfer principle for Levi-degenerate sources consumes as a hypothesis.

Background

The rigidity of holomorphic mappings between bounded domains has been a central theme of several complex variables since Poincaré. A benchmark is proper holomorphic maps between unit balls Bn→BN\mathbb{B}^n\to\mathbb{B}^N (maps whose preimage of every compact set is compact; between bounded domains this forces the boundary to be mapped to the boundary): Huang proved that a map which is C2C^2-smooth up to the boundary with n≤N≤2n−2n\le N\le 2n-2 is a totally geodesic (linear) embedding. The key tool, now called Huang's Lemma, states that if holomorphic functions φj,ψj\varphi_j,\psi_j (1≤j≤k≤n−11\le j\le k\le n-1) vanish at the origin and satisfy ∑j=1kφj(z)ψj(z)=∥z∥2H(z,zˉ)\sum_{j=1}^{k}\varphi_j(z)\psi_j(z)=\|z\|^2 H(z,\bar z) with HH real-analytic, then H≡0H\equiv 0. The invariant controlling such identities is the Hermitian rank: a real-analytic function has Hermitian rank at most p+qp+q when it can be written as ∑i=1p∣fi(z)∣2−∑j=1q∣gj(z)∣2\sum_{i=1}^{p}|f_i(z)|^2-\sum_{j=1}^{q}|g_j(z)|^2 with holomorphic fi,gjf_i,g_j, and the minimal such p+qp+q is its rank (a notion originating in Hilbert's 17th problem and its sums-of-squares analogues). Huang's Lemma says a multiplier of ∥z∥2\|z\|^2 is forced to vanish in the low-term range; Xiao proved the first non-degenerate version: at term count k=nk=n, either H≡0H\equiv 0 or HH has rank one and the tuples φ,ψ\varphi,\psi are linear up to holomorphic factors.

The paper under consideration (Gao) works in a coordinate-free geometric framework. Let Cr,s,t\mathbb{C}^{r,s,t} denote Cr+s+t\mathbb{C}^{r+s+t} with the standard, possibly indefinite and degenerate Hermitian form ⟨z,w⟩r,s,t=∑i≤rziwˉi−∑r<i≤r+sziwˉi\langle z,w\rangle_{r,s,t}=\sum_{i\le r}z_i\bar w_i-\sum_{r<i\le r+s}z_i\bar w_i (the last tt coordinates enter trivially), and let Pr,s,tP^{r,s,t} be its projectivization. The generalized ball Br,s,tB^{r,s,t} is its set of positive points; the boundary, consisting of null points, is a CR hypersurface (a real hypersurface of complex space whose tangent spaces carry a maximal complex subspace — the natural setting for boundary rigidity questions) which is Levi-degenerate when t>0t>0 (the Levi form, the intrinsic pseudoconvexity curvature of such a hypersurface, is here the Hermitian form itself, which has a tt-dimensional kernel along the boundary). A local orthogonal pair is a pair of holomorphic maps (φ,ψ)(\varphi,\psi) from an open subset of Pr,s,tP^{r,s,t} to Pr′,s′,t′P^{r',s',t'} such that φ(p)⊥ψ(q)\varphi(p)\perp\psi(q) with respect to the target form whenever p⊥qp\perp q with respect to the source form; this is the projective incarnation of a pair of Segre maps (the Segre variety of a boundary point is the set of points joined to it by complex lines lying in the ambient hypersurface — a standard local invariant that linearizes CR mapping questions), and the diagonal case φ=ψ=f\varphi=\psi=f is a local orthogonal map, the coordinate-free model of a local CR map between hyperquadrics. A pair is null if φ(p)⊥ψ(q)\varphi(p)\perp\psi(q) for all p,qp,q (a trivial solution), standard if it is induced by a linear conformal pair of the underlying Hermitian spaces, and quasi-standard if it splits as a direct sum of a standard part and a null part. In homogeneous coordinates an orthogonal pair satisfies a generalized Huang equation ∑j=1r′φjψj−∑j=r′+1r′+s′φjψj=∥z∥r,s,t2H(z,zˉ)\sum_{j=1}^{r'}\varphi_j\psi_j-\sum_{j=r'+1}^{r'+s'}\varphi_j\psi_j=\|z\|^2_{r,s,t}H(z,\bar z), and the multiplier HH — determined up to a product of two holomorphic functions — completely characterizes the two rigid alternatives: the pair is null if and only if H≡0H\equiv 0, and quasi-standard if and only if H=h1(z)h2(z)H=h_1(z)h_2(z) has Hermitian rank one.

Gao's main theorem extends Huang's Lemma to the sharp term range for arbitrary signature: if r+s≤n′≤2(r+s)−3r+s\le n'\le 2(r+s)-3 and H≢0H\not\equiv 0, then H=h1h2H=h_1h_2 and the tuples are partially linear, φ=B(h1z1,…,h1zr+s,Φ1,…,Φq)\varphi=B(h_1z_1,\dots,h_1z_{r+s},\Phi_1,\dots,\Phi_q) and ψ=C(h2z1,…,h2zr+s,Ψ1,…,Ψq)\psi=C(h_2z_1,\dots,h_2z_{r+s},\Psi_1,\dots,\Psi_q), with constant matrices satisfying CTB=Hr,s,qC^TB=H_{r,s,q} and q=n′−r−sq=n'-r-s. A companion transfer theorem deduces rigidity for Levi-degenerate sources from the non-degenerate case: if all local orthogonal pairs from Pr,sP^{r,s} to Pr′,s′P^{r',s'} are quasi-standard or null, then the same holds from Pr,s,tP^{r,s,t} for every t,t′t,t'. The numerical bound is sharp: at n′=2(r+s)−2n'=2(r+s)-2 the generalized Whitney map of Huang–Xiao satisfies the equation with multiplier (∣z1∣2+∣zn∣2)2(|z_1|^2+|z_n|^2)^2 of Hermitian rank three (throughout, n=r+sn=r+s denotes the non-degenerate source dimension), so the rank-one conclusion, and with it quasi-standard rigidity, fails. The known rigidity patches are restricted: Gao's earlier theorem covers pairs from Pr,sP^{r,s} into positive-definite targets Pn′,0P^{n',0} with n′≤2(r+s)−3n'\le 2(r+s)-3; Gao–Ng cover local orthogonal maps when min⁡{r′,s′}≤min⁡{r,s}\min\{r',s'\}\le\min\{r,s\} (with r,s≥2r,s\ge2), when min⁡{r′,s′}≤2min⁡{r,s}−2\min\{r',s'\}\le 2\min\{r,s\}-2 (with t=0t=0), and when r′+s′≤2(r+s)−3r'+s'\le 2(r+s)-3 (with t=0t=0); Huang–Xiao independently proved the orthogonal-map transfer theorem for degenerate sources. No structural description exists at the borderline n′=2(r+s)−2n'=2(r+s)-2 or for general indefinite targets outside these ranges — precisely the input that further applications of the transfer principle require as a hypothesis.

Problem Statement

Let r,s,t≥0r,s,t\ge 0 with r+s≥2r+s\ge 2, and set n′=2(r+s)−2n'=2(r+s)-2. Classify the local orthogonal pairs (and, as the diagonal case, the local orthogonal maps) from Pr,s,tP^{r,s,t} into the positive-definite target Pn′,0P^{n',0}, up to the natural equivalence generated by linear conformal changes of source and target (that is, by linear conformal pairs in the sense of Definition 2.2 of the source paper: pairs of linear maps Φ,Ψ\Phi,\Psi satisfying ⟨Φ(z),Ψ(w)⟩n′,0=λ⟨z,w⟩r,s,t\langle\Phi(z),\Psi(w)\rangle_{n',0}=\lambda\langle z,w\rangle_{r,s,t} for some λ∈R∗\lambda\in\mathbb{R}^*) and by the direct-sum splitting into standard and null parts. Concretely, determine whether every such pair is null, quasi-standard, or equivalent to a generalized Whitney-type pair as in Example 1.2 of the source paper (the pair whose multiplier is the Hermitian-rank-three polynomial (∣z1∣2+∣zn∣2)2(|z_1|^2+|z_n|^2)^2 described in the background), or whether further local structures occur at this borderline codimension; in the non-degenerate case t=0t=0 this amounts to classifying the solutions ({φj}j=1n′,{ψj}j=1n′,H≢0)(\{\varphi_j\}_{j=1}^{n'},\{\psi_j\}_{j=1}^{n'},H\not\equiv 0) of the generalized Huang equation ∑j=1n′φj(z)ψj(z)=∥z∥r,s2H(z,zˉ)\sum_{j=1}^{n'}\varphi_j(z)\psi_j(z)=\|z\|^2_{r,s}H(z,\bar z) at term count n′=2(r+s)−2n'=2(r+s)-2, including the possible Hermitian ranks of the multiplier, the uniqueness and moduli of the holomorphic factors, and the structure of the complementary components Φi,Ψi\Phi_i,\Psi_i. As the linked second component of the same objective — the missing hypothesis for the transfer theorem (Theorem 1.3 of the source) — determine for which signature pairs (r′,s′)(r',s') and which target dimensions beyond 2(r+s)−32(r+s)-3 every local orthogonal pair from the non-degenerate source Pr,sP^{r,s} to Pr′,s′P^{r',s'} is quasi-standard or null, and classify the exceptions when this dichotomy fails.

References

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