The GIT Boundary of Quintic Threefolds

Author: Yasutaka Shibata Version 2

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Overview

This paper determines the strictly semistable boundary in the Geometric Invariant Theory (GIT) quotient for quintic threefolds, that is, degree-five hypersurfaces X ⊂ ℙ4. The group G = SL(5) acts naturally on ℙ(W), where W = Sym55. Writing MGIT = ℙ(W)ss // G and π for the quotient map, the boundary studied here is π(ℙ(W)ss ∖ ℙ(W)s). It is not the entire complement of the smooth-quintic locus in the GIT quotient.

MGIT = Θ1 ∪ ⋯ ∪ Θ21.

21 irreducible boundary components

The 38 maximal strictly torus-semistable monomial supports give exactly 21 quotient-side components. Distinct components are neither equal nor contained in one another.

Dimensions from 1 to 24

Every component has an explicit polystable weight-zero normal-form family. Its generic connected projective stabilizer is a one-dimensional torus; these 21 tori are pairwise nonconjugate.

11 isolated local families

For general closed-orbit representatives, the isolated singularities form exactly 11 weighted-homogeneous local families. Their normalized weights occur in Yonemura’s list.

Global minimal exponent 1

In every component, a general closed-orbit representative has global minimal exponent α~(X) = 1 = (4 + 1)/5, the critical value for quintics in 4.

Source: Version 2, Theorem A (p. 2).

Throughout this overview, “general” means on the nonempty Zariski-open parameter loci specified in the paper. The normal-form, stabilizer, and singularity assertions are not claims about every parameter specialization; the displayed normal-form parameterizations are not asserted to be unique.

The 21 quotient-side boundary components

Why 38 supports give 21 components

The Hilbert–Mumford calculation enumerates 38 maximal strictly semistable monomial supports for the diagonal maximal torus, up to coordinate permutation. Their G-saturations cover the strictly semistable locus, but this support-indexed cover is not yet an irreducible-component decomposition of the quotient.

Zero-weight reduction shows that reversing a supporting half-space does not change its quotient image: Φ(r) = Φ(−r). Reversal pairs 34 of the support labels into 17 pairs and fixes four labels, namely 13, 14, 19, and 36. Thus 38 = 17 × 2 + 4 oriented supports yield 17 + 4 = 21 quotient families.

Version 2: supports and components are counted separately. The number 38 counts oriented maximal supports. The number 21 counts the irreducible components of the strictly semistable boundary in the GIT quotient, after the opposite-support identifications and the proof of pairwise non-inclusion.

Sources: Section 4: zero-weight reduction and supporting-hyperplane invariance; Section 6: the component theorem.

Component catalog

In the following table, Φk denotes a support-indexed quotient family, k(a) is the chosen normal-form case, and the primitive normal ra defines the generic connected projective stabilizer Ha = λra(Gm). The last column is the quotient dimension.

The 21 components, with support identifications and dimensions
Component Support-indexed image k(a) Supporting normal ra Dimension
Θ1 Φ1 = Φ26 1 (36, 1, −4, −9, −24) 1
Θ2 Φ2 = Φ27 2 (27, 2, −3, −8, −18) 2
Θ3 Φ3 = Φ33 3 (3, 0, 0, −1, −2) 6
Θ4 Φ4 = Φ21 4 (24, 9, −6, −11, −16) 2
Θ5 Φ5 = Φ24 5 (21, 6, −4, −9, −14) 3
Θ6 Φ6 = Φ28 6 (18, 3, −2, −7, −12) 5
Θ7 Φ7 = Φ18 7 (5, 1, 0, −2, −4) 2
Θ8 Φ8 = Φ16 8 (4, 2, −1, −2, −3) 2
Θ9 Φ9 = Φ22 9 (19, 4, −1, −6, −16) 4
Θ10 Φ10 = Φ34 10 (12, 2, −3, −3, −8) 8
Θ11 Φ11 = Φ25 11 (14, 4, −1, −6, −11) 6
Θ12 Φ12 = Φ17 12 (13, 8, −2, −7, −12) 5
Θ13 Φ13 13 (3, 2, 0, −2, −3) 4
Θ14 Φ14 14 (4, 1, 0, −1, −4) 4
Θ15 Φ15 = Φ30 15 (9, 4, −1, −6, −6) 9
Θ16 Φ19 19 (2, 1, 0, −1, −2) 8
Θ17 Φ20 = Φ31 20 (8, 3, −2, −2, −7) 11
Θ18 Φ23 = Φ38 23 (4, −1, −1, −1, −1) 19
Θ19 Φ29 = Φ35 29 (6, 1, 1, −4, −4) 15
Θ20 Φ32 = Φ37 32 (3, 3, −2, −2, −2) 18
Θ21 Φ36 36 (1, 0, 0, 0, −1) 24

Source: Version 2, Table 2 (p. 5). The component index a and the support-case label k(a) differ from component 16 onward.

The four largest components are Θ21 (dimension 24), Θ18 (19), Θ20 (18), and Θ19 (15). The comparison in Section 7 identifies these with Lakhani’s four first-level families. The other 17 are additional irreducible components, not contained in their union. See Section 7.

Closed orbits and the non-inclusion argument

Weight-zero limits and Luna’s centralizer reduction produce explicit polystable normal forms. Exact rank certificates then show that the generic connected projective stabilizers are precisely the one-dimensional tori listed above. Their pairwise nonconjugacy, together with Luna’s étale slice theorem, rules out containments between distinct quotient families. The component theorem therefore uses stabilizers, not merely a comparison of dimensions.

Sources: Section 5, Section 6, and Appendix A. The 21 normal-form equations and their genericity conditions are collected in Table 1 (pp. 3–4).

Singularities and the minimal exponent

For a general closed-orbit representative in each component, the paper computes the saturated Jacobian scheme and its local analytic stratification. Positive-dimensional singular supports include configurations of lines, smooth conics, cuspidal plane curves, a plane, and a smooth quartic surface. The catalog distinguishes generic transverse structures from special strata where the transverse model changes, and records all isolated singular points.

Source: Version 2, Table 3 (pp. 6–7); the component-by-component calculations are in Appendix B.

The 11 isolated weighted-homogeneous local families

The table below summarizes the integral weights, Milnor numbers, Yonemura row numbers, and occurrences of the 11 families. Here P0 = (1 : 0 : 0 : 0 : 0) and P = (0 : 0 : 0 : 0 : 1), in the coordinates of the normal forms. The defining local equations and parameter conditions are given in Table 4 and Definitions 8.1–8.11 of the paper.

Isolated-family data from Table 4
Integral weights (w1, w2, w3, w4; D) Milnor number μ Yonemura No. Component / point
(1, 1, 1, 1; 4) 81 1 Θ18: P0
(7, 8, 9, 12; 36) 87 52 Θ1: P0
(5, 6, 7, 9; 27) 88 84 Θ2: P0
(3, 3, 4, 5; 15) 88 15 Θ3: P0
(2, 3, 3, 4; 12) 90 2 Θ10: P0
(3, 4, 5, 6; 18) 91 53 Θ6: P0
(4, 5, 7, 9; 25) 96 86 Θ7: P0
(3, 4, 5, 7; 19) 96 94 Θ9: P0
(1, 1, 1, 2; 5) 96 21 Θ21: P0, P
(1, 1, 2, 2; 6) 100 3 Θ19: P0
(3, 4, 5, 8; 20) 102 62 Θ14: P0, P

Source: Version 2, Table 4 (pp. 7–8).

“Yonemura-type” is a statement about normalized weights. Each normalized weight system occurs in Yonemura’s Table 2.2. This does not assert that every member of one of these local families is analytically equivalent to the particular polynomial displayed in that list. The occurrence-and-exhaustion statement concerns general closed-orbit representatives on the quintic GIT boundary. See the explanation following Table 4.

The extremal value

Every isolated family above has w1 + w2 + w3 + w4 = D, so its local minimal exponent is one. The local analysis along the positive-dimensional singular loci shows that no stratum forces a value below one, while at least one stratum in every component attains one. Consequently, for a general Xa = V(Fa),

α~(Xa) = 1 = (4 + 1)/5, a = 1, …, 21.

“Extremal” refers to equality with the critical value (n + 1)/d for degree-five hypersurfaces in 4.

Sources: Introduction (pp. 10–11) and Appendix B.

Guide to Version 2

All references below point to the corresponding pages of the Version 2 PDF.

Where to find the statements, catalogs, and proofs
PDF locationContents
Theorem A (p. 2) The complete boundary classification and its five main assertions.
Table 1 (pp. 3–4) The 21 polystable weight-zero normal-form families, with equations and genericity conditions.
Table 2 (p. 5) Quotient components, support identifications, supporting normals, generic stabilizers, and dimensions.
Table 3 (pp. 6–7) Generic singular supports, transverse structures, special strata, and isolated families for each component.
Table 4 (pp. 7–8) The 11 isolated local families: equations, integral weights, Milnor numbers, and component occurrences.
Sections 2–6 (pp. 11–32) Support enumeration, the boundary cover, quotient-side identifications, closed orbits, stabilizers, and non-inclusion.
Section 7 (pp. 33–36) Comparison with Lakhani’s classification and the four largest components.
Section 8 (pp. 37–46) The component-indexed singularity catalog and minimal-exponent conclusion.
Appendix A (from p. 47) The 38 support-by-support constructions of polystable normal forms.
Appendix B (from p. 116) The 21 component-by-component calculations of singular schemes, local analytic types, and minimal exponents.