Polyhedra, Moduli,
and Quantum Geometry

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  1. 7.1 The fixed-curvature leaf at the Euclidean end
  2. 7.2 The same periods describe hypergeometric functions and developed edges
  3. 7.3 Collision angles and the lattice conditions
  4. 7.4 Four equal deficits and elliptic periods

7 Euclidean shapes and Deligne–Mostow periods

7.1 The fixed-curvature leaf at the Euclidean end

Fix n≥4n\ge4 and real numbers 0<μi<1,∑i=1nμi=2.0<\mu_i<1,\qquad \sum_{i=1}^n\mu_i=2.(7.1) The Euclidean cone opening at the iith marked point is 2π(1−μi)2\pi(1-\mu_i), so 2πμi2\pi\mu_i is its curvature deficit. A conformal sphere XX with these marked points carries a unique such flat metric up to multiplication by a positive constant. In a coordinate with all marks finite it has the explicit form gE,μ=C∏i|w−pi|−2μi|⁡dw|2.g_{\mathrm E,\mu}=C\prod_i|w-p_i|^{-2\mu_i}|\mathop{}\!\mathrm dw|^2.(7.2) The sum condition makes infinity a regular point. Near pip_i, radial integration gives a cone of opening 2π(1−μi)2\pi(1-\mu_i). Thus the space of oriented, labeled Euclidean cone spheres with these deficits, up to similarity, has underlying complex manifold ℳ0,n\mathcal M_{0,n}.

Alexandrov realization identifies these metrics with convex Euclidean polyhedral surfaces, allowing doubled planar polygons. This is the fixed-deficit space on which Thurston constructs his complex hyperbolic metric [97; 57]. The qualification “fixed deficits” is essential: all Euclidean polyhedra with nn vertices, up to similarity, form a space of real dimension 3n−73n-7, whereas the fixed-deficit leaf has real dimension 2n−62n-6. The full space of compact hyperbolic nn-vertex polyhedra has dimension 3n−63n-6; its fixed-cone-angle leaves again have dimension 2n−62n-6. The ideal locus has dimension 2n−62n-6. These dimension counts apply on the generic strata; changes of combinatorics and flattened realizations require the usual cell structure. Figure 2 distinguishes these geometric regimes and the rescaled Euclidean limit.

Euclidean, compact, ideal, and hyperideal regimes
Figure 2. Local pictures for the geometric regimes. The three Klein-model drawings are planar sections illustrating the location of vertices; the ochre segments are polar truncations in the hyperideal case. The Euclidean picture represents a tangent-scale limit after shrinking and rescaling. These drawings do not assert a single global deformation through all four regimes with arbitrary prescribed data.

7.2 The same periods describe hypergeometric functions and developed edges

Define the multivalued differential ηp(w)=∏i(w−pi)−μi⁡dw.\eta_p(w)=\prod_i(w-p_i)^{-\mu_i}\,\mathop{}\!\mathrm dw.(7.3) Its branches differ by unit complex numbers. It therefore defines a twisted cohomology class for a rank-one unitary local system on the punctured sphere. The relevant twisted cohomology space has complex dimension n−2n-2, and its Hermitian intersection form HH has signature (1,n−3)(1,n-3), with the convention that the class of ηp\eta_p has positive norm. In a local basis of twisted cycles or regularized relative arcs, the coordinates Zj(p)=∫γjηpZ_j(p)=\int_{\gamma_j}\eta_p(7.4) are the hypergeometric periods of Deligne–Mostow [53]. Projectivizing their positive line gives a local map to ℂℍn−3\mathbb{CH}^{n-3}. Analytic continuation produces projective unitary monodromy.

Thurston’s Euclidean construction uses exactly the same coordinates. The local developing map is F(w)=∫wηp.F(w)=\int^w\eta_p. Hence a developed edge vector is an integral of ηp\eta_p along the corresponding arc. Cutting along a tree produces a Euclidean polygon whose edge vectors are periods, and whose area is the Hermitian form in these periods. Normalize HH by this area pairing. Then, more intrinsically, 𝒜(p)=i2∫ℙ1ηp∧ηp¯=H(Z(p),Z(p)).\mathcal A(p)=\frac{i}{2}\int_{\mathbb P^1}\eta_p\wedge\overline{\eta_p} =H(Z(p),Z(p)).(7.5) Multiplication of all periods by a nonzero complex number changes only the scale and rotation of the developed surface. Quotienting by this action is precisely the projectivization in the Deligne–Mostow construction.

Thus the connection is an equality of geometric structures: the hypergeometric periods are the developed edge vectors, and the Hermitian intersection pairing is the area pairing. Kojima proves that the two constructions, with labels retained, are canonically isometric [66, Lemmas 4.1–4.2 and Theorem 4.3]. The scalar used for the Hermitian intersection pairing varies between sources; fixing it by (7.5) removes that ambiguity, and a constant scalar does not change the projective metric. Throughout this monograph the complex hyperbolic metric has holomorphic sectional curvature −1-1. Its Kähler form, in the preceding local period coordinates, is ωCH=−2i∂∂‾log⁡𝒜.\omega_{\mathrm{CH}}=-2i\,\partial\bar\partial\log\mathcal A.(7.6) A holomorphic change of local scale for ηp\eta_p does not affect this form. On a complex line in the ball, 𝒜=1−|z|2\mathcal A=1-|z|^2 gives ⁡ds2=4|⁡dz|2/(1−|z|2)2\mathop{}\!\mathrm ds^2=4|\mathop{}\!\mathrm dz|^2/(1-|z|^2)^2, which checks the curvature normalization directly. A curvature-−4-4 convention would divide the form by 44 and the volume in complex dimension dd by 4d4^d.

If the weights are rational, choose their least common denominator qq, so μi=mi/q\mu_i=m_i/q. The compact normalization of the connected cyclic cover yq=∏i(w−pi)miy^q=\prod_i(w-p_i)^{m_i} makes ηp=⁡dw/y\eta_p=\mathop{}\!\mathrm dw/y a single-valued holomorphic differential. Under the deck transformation y↦e2πi/qyy\mapsto e^{2\pi i/q}y it has eigenvalue e−2πi/qe^{-2\pi i/q}. The corresponding eigenspace in the ordinary cohomology of this cover realizes the twisted cohomology. This gives a further useful interpretation in terms of periods of algebraic curves; it does not require the monodromy group to be a lattice.

7.3 Collision angles and the lattice conditions

Suppose two marks of total weight μi+μj<1\mu_i+\mu_j<1 collide, with local separation δ\delta, while the other marks remain distinct and away from the collision. After fixing a branch, rescaling the integration variable in their vanishing period gives Zij(δ)=Cδ1−μi−μj(1+O(δ)),C≠0.Z_{ij}(\delta)=C\delta^{\,1-\mu_i-\mu_j}(1+O(\delta)),\qquad C\ne0.(7.7) The transverse complex hyperbolic cone angle is consequently 2π(1−μi−μj)2\pi(1-\mu_i-\mu_j). Deligne–Mostow’s condition INT is (1−μi−μj)−1∈ℤ>0for every pair with μi+μj<1.(1-\mu_i-\mu_j)^{-1}\in\mathbb Z_{>0} \quad\text{for every pair with }\mu_i+\mu_j<1.(7.8) Under this condition the completion by finite-distance collisions has orbifold universal cover ℂℍn−3\mathbb{CH}^{n-3}, and the monodromy is a lattice. Cusps remain at infinite distance. For the half-integral variant, fix a block of equal-weight marks and permit every permutation within that block. Interchanging two of its marks sends δ\delta to −δ-\delta; the quotient coordinate is δ2\delta^2, so the transverse angle is halved. Mostow’s Σ\SigmaINT condition is therefore (1−μi−μj)−1∈{12ℤ>0,i,j both in the specified block,ℤ>0,otherwise,μi+μj<1.(1-\mu_i-\mu_j)^{-1}\in \begin{cases} \tfrac12\mathbb Z_{>0},&i,j\text{ both in the specified block},\\ \mathbb Z_{>0},&\text{otherwise}, \end{cases} \qquad \mu_i+\mu_j<1. Mostow’s theorem gives an orbifold uniformization for that permutation quotient [81, Sections 1–3]; the labeled completion need not itself be an orbifold when a reciprocal is a nonintegral half-integer. Thurston gives the corresponding criterion when all equal-weight permutations are allowed [97, Theorem 0.2].

When μi+μj=1\mu_i+\mu_j=1, the collision is a cusp rather than a finite cone-angle divisor; logarithmic periods and parabolic monodromy enter. For general real weights satisfying (7.1), the local complex hyperbolic geometry and its finite volume still exist [97, Theorem 0.2]. One must not infer a lattice quotient for arbitrary weights. Conversely, INT and Σ\SigmaINT are the classical sufficient uniformization conditions, not a claim to classify every exceptional discrete hypergeometric monodromy group. Our volumes retain all labels; a quotient by allowed equal-weight permutations changes the quotient and the volume factors.

7.4 Four equal deficits and elliptic periods

For n=4n=4 and μi=1/2\mu_i=1/2, put the marks at 0,1,z,∞0,1,z,\infty. Then η=⁡dww(w−1)(w−z),Ez:y2=w(w−1)(w−z).\eta=\frac{\mathop{}\!\mathrm dw}{\sqrt{w(w-1)(w-z)}},\qquad E_z:\ y^2=w(w-1)(w-z).(7.9) The Euclidean cone sphere is the flat pillowcase quotient of this elliptic curve. The ratio of two periods gives a coordinate τ∈ℍ\tau\in\mathbb H. For 0<z<10<z<1, one choice is τ(z)=iK(1−z)K(z),K(z)=∫0π/2⁡du1−zsin⁡2u.\tau(z)=i\frac{K(1-z)}{K(z)},\qquad K(z)=\int_0^{\pi/2}\frac{\mathop{}\!\mathrm du}{\sqrt{1-z\sin^2u}}.(7.10) Here zz is the elliptic parameter, not its square root. The inverse map is the modular lambda function. Projective monodromy is PΓ(2)=Γ(2)/{±I}\mathrm P\Gamma(2)=\Gamma(2)/\{\pm I\}, and the labeled moduli space is the thrice-punctured sphere with curvature-−1-1 area 2π2\pi. The action of S4S_4 on the cross-ratio has the Klein four-group as its kernel. Its effective quotient therefore has degree 66, and is the modular orbifold of area π/3\pi/3; dividing the labeled area by 2424 would instead retain the ineffective stabilizer [66, Example 2.1 and Section 5]. This is the flat endpoint of the equal-angle torus–sphere correspondence in Section 6.