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Gushel-Mukai Threefolds

Updated 5 March 2026
  • Gushel-Mukai threefolds are smooth complex Fano threefolds of Picard rank one, degree 10, and index 1, constructed via codimension‐2 sections or double covers of Grassmannians.
  • They display deep connections to Hodge theory, EPW sextics, and derived categories, offering pivotal insights into Torelli problems and rationality.
  • Their 10-dimensional irreducible moduli space underscores applications in birational geometry, stability conditions, and categorical resolutions.

A Gushel–Mukai threefold (GM threefold) is a smooth complex Fano threefold of Picard rank one, index one, and degree ten. These varieties possess rich geometric, Hodge-theoretic, and categorical structures that connect them to the geometry of Grassmannians, K3 surfaces, hyperkähler manifolds, Eisenbud–Popescu–Walter (EPW) sextics, and modern developments in derived categories and Bridgeland stability. GM threefolds serve as a central example in Fano geometry and categorical birational theory, providing fertile ground for Torelli-type theorems, moduli constructions, and the study of rationality.

1. Geometric Constructions and Classification

A GM threefold XX is realized as either:

  • an ordinary GM threefold: a smooth codimension-2 linear section of the Grassmannian Gr(2,5)\mathrm{Gr}(2,5) in its Plücker embedding, cut by a quadric,
  • or a special GM threefold: a double cover of a quintic del Pezzo threefold (a 3-dimensional linear section of Gr(2,5)\mathrm{Gr}(2,5)) branched along a smooth ordinary GM surface (degree-10 K3 surface).

Explicitly, let V5V_5 be a 5-dimensional complex vector space and Gr(2,V5)⊂P9\mathrm{Gr}(2,V_5)\subset \mathbb{P}^9 its Plücker embedding. For the ordinary case, one selects a codimension-2 linear subspace W⊂∧2V5W\subset \wedge^2 V_5 and a quadric QQ in P(W)\mathbb{P}(W), obtaining: X=Gr(2,V5)∩P(W)∩QX = \mathrm{Gr}(2,V_5) \cap \mathbb{P}(W) \cap Q For the special case, M=Gr(2,V5)∩P(W)M = \mathrm{Gr}(2,V_5)\cap \mathbb{P}(W) is a Fano threefold (Gr(2,5)\mathrm{Gr}(2,5)0), Gr(2,5)\mathrm{Gr}(2,5)1 a quadric section (K3 surface), and Gr(2,5)\mathrm{Gr}(2,5)2 is the double cover Gr(2,5)\mathrm{Gr}(2,5)3 branched over Gr(2,5)\mathrm{Gr}(2,5)4.

Both types yield smooth Fano threefolds of degree Gr(2,5)\mathrm{Gr}(2,5)5, index Gr(2,5)\mathrm{Gr}(2,5)6, and genus Gr(2,5)\mathrm{Gr}(2,5)7 (since Gr(2,5)\mathrm{Gr}(2,5)8). The Mukai classification theorem asserts that all smooth Fano threefolds with these invariants are GM threefolds (Bayer et al., 27 Jan 2025, Debarre et al., 2015).

The moduli space of such varieties is irreducible and 10-dimensional, parameterized by Lagrangian data Gr(2,5)\mathrm{Gr}(2,5)9, where Gr(2,5)\mathrm{Gr}(2,5)0 is a Lagrangian subspace, Gr(2,5)\mathrm{Gr}(2,5)1 a hyperplane, and Gr(2,5)\mathrm{Gr}(2,5)2 satisfies a transversality condition with Gr(2,5)\mathrm{Gr}(2,5)3 (Debarre et al., 2015). Special GM threefolds correspond to an additional degeneracy in these data.

2. Hodge Theory, Periods, and Rationality

The Hodge diamond of a smooth GM threefold Gr(2,5)\mathrm{Gr}(2,5)4 is:

  • Gr(2,5)\mathrm{Gr}(2,5)5
  • Gr(2,5)\mathrm{Gr}(2,5)6
  • Gr(2,5)\mathrm{Gr}(2,5)7

The third cohomology group Gr(2,5)\mathrm{Gr}(2,5)8 is pure of type Gr(2,5)\mathrm{Gr}(2,5)9 and of dimension V5V_50. The intermediate Jacobian V5V_51 is a principally polarized abelian variety of dimension V5V_52, and the period map sending V5V_53 to V5V_54 is a central tool in studies of Torelli-type problems and rationality (Debarre, 2020, Lin et al., 9 Jul 2025).

The period map for ordinary GM threefolds is generically V5V_55-to-V5V_56 on its image, with a 2-dimensional fiber arising from extra deformations that keep the Hodge structure fixed; this corresponds to a 2-dimensional kernel in the differential of the period map (Lin et al., 9 Jul 2025). For special GM threefolds, the invariant part of the infinitesimal period map is injective by Hodge-theoretic and categorical arguments.

A pivotal result in irrationality asserts that the intermediate Jacobian of a general GM threefold cannot be isogenous to a product of Jacobians of curves, and in certain cases the action of finite groups such as V5V_57 on V5V_58 prohibits rationality (Debarre et al., 2021). Unirationality is classical for all smooth GM threefolds, but rationality occurs only in particular singular or specialized situations (Debarre et al., 2015).

3. EPW Sextics and Moduli Connections

To each GM threefold (or Gushel-Mukai surface) is associated a Lagrangian subspace V5V_59, giving rise to an EPW sextic Gr(2,V5)⊂P9\mathrm{Gr}(2,V_5)\subset \mathbb{P}^90 in Gr(2,V5)⊂P9\mathrm{Gr}(2,V_5)\subset \mathbb{P}^91 defined by

Gr(2,V5)⊂P9\mathrm{Gr}(2,V_5)\subset \mathbb{P}^92

The singular locus Gr(2,V5)⊂P9\mathrm{Gr}(2,V_5)\subset \mathbb{P}^93 parametrizes points where this intersection has dimension at least 2. O'Grady's theory supplies a canonical double cover Gr(2,V5)⊂P9\mathrm{Gr}(2,V_5)\subset \mathbb{P}^94 branched along Gr(2,V5)⊂P9\mathrm{Gr}(2,V_5)\subset \mathbb{P}^95, which for general Gr(2,V5)⊂P9\mathrm{Gr}(2,V_5)\subset \mathbb{P}^96 is a smooth irreducible holomorphic symplectic variety of K3Gr(2,V5)⊂P9\mathrm{Gr}(2,V_5)\subset \mathbb{P}^97-type (Liu et al., 15 Dec 2025).

Period partners (GM threefolds with the same Gr(2,V5)⊂P9\mathrm{Gr}(2,V_5)\subset \mathbb{P}^98 but different Gr(2,V5)⊂P9\mathrm{Gr}(2,V_5)\subset \mathbb{P}^99) and duals (W⊂∧2V5W\subset \wedge^2 V_50 vs.\ W⊂∧2V5W\subset \wedge^2 V_51) are always birational in dimension three, as are their period loci in the moduli space (Debarre et al., 2015). The geometry of lines and conics on W⊂∧2V5W\subset \wedge^2 V_52 is controlled by the associated EPW sextic.

Moduli functors for stable objects in the derived category (see below) provide further bridges between GM varieties and the geometry of their EPW data (Liu et al., 15 Dec 2025). In the case of special GM threefolds, the double EPW surface W⊂∧2V5W\subset \wedge^2 V_53 is realized as a Bridgeland moduli space of semistable objects in the Kuznetsov component (Liu et al., 15 Dec 2025).

4. Derived Categories, Categorical Torelli, and Moduli of Stable Objects

For any GM threefold W⊂∧2V5W\subset \wedge^2 V_54, the bounded derived category W⊂∧2V5W\subset \wedge^2 V_55 admits a semiorthogonal decomposition

W⊂∧2V5W\subset \wedge^2 V_56

where W⊂∧2V5W\subset \wedge^2 V_57 is the dual tautological bundle, and the Kuznetsov component W⊂∧2V5W\subset \wedge^2 V_58 is an admissible subcategory behaving as a "fractional Calabi–Yau" category with Serre functor W⊂∧2V5W\subset \wedge^2 V_59; for special GM threefolds, QQ0 carries an involution from the covering and is thus a noncommutative analogue of a K3 (Pertusi et al., 2021, Feyzbakhsh et al., 2023).

Moduli spaces of Bridgeland-stable objects in QQ1, constructed via double tilting of the heart of QQ2 and an explicitly defined central charge, realize many natural geometric loci:

  • For special GM threefolds, the moduli space QQ3 coincides with the double EPW surface QQ4, while QQ5 corresponds to QQ6 (Liu et al., 15 Dec 2025).
  • For ordinary GM threefolds, the minimal model QQ7 of the Fano surface of conics is isomorphic to a Bridgeland moduli space in QQ8 (Zhang, 2020).

A refined categorical Torelli theorem holds: for a general ordinary GM threefold, the Kuznetsov component together with the image of the tautological bundle determines QQ9 up to isomorphism (Jacovskis et al., 2021, Feyzbakhsh et al., 2023). Furthermore, for special GM threefolds (under genericity conditions on lines/conics), P(W)\mathbb{P}(W)0 fully captures the isomorphism class (Liu et al., 15 Dec 2025).

The group of Fourier–Mukai autoequivalences of P(W)\mathbb{P}(W)1 for general P(W)\mathbb{P}(W)2 coincides with the product of P(W)\mathbb{P}(W)3 (the automorphism group of P(W)\mathbb{P}(W)4), the Serre functor, and the shift functor, highlighting the rigidity of this construction for generic GM threefolds (Feyzbakhsh et al., 2023).

5. Stability Conditions, Wall-Crossing, and Applications

Bridgeland stability conditions on P(W)\mathbb{P}(W)5 have been explicitly constructed by successive tilting (first slope, then tilt) of P(W)\mathbb{P}(W)6, yielding hearts and central charges compatible with the Serre functor; these conditions give a unique P(W)\mathbb{P}(W)7-orbit of Serre-invariant stability conditions (Pertusi et al., 2021).

Wall-crossing in these stability conditions controls birational modifications of moduli spaces of stable objects, such as the flop wall for length-2 subschemes (Hilbert schemes) and divisorial contractions of the Hilbert scheme of twisted cubics on special GM threefolds (Liu et al., 15 Dec 2025, Zhang, 2020). Many of these spaces are proven to be projective, smooth (in the generic case), and holomorphic symplectic.

The action of the Serre functor on P(W)\mathbb{P}(W)8 is tightly intertwined with stability conditions, and in the case of special GM fourfolds, the Kuznetsov component of the threefold lifts to the equivariant category, providing a construction of stability conditions on higher-dimensional analogues (Pertusi et al., 2021).

6. Birational Geometry, Automorphisms, and Categorical Resolutions

GM threefolds exhibit intricate birational geometry: any two birationally equivalent GM threefolds are either period partners or duals (sharing an EPW Lagrangian P(W)\mathbb{P}(W)9 or X=Gr(2,V5)∩P(W)∩QX = \mathrm{Gr}(2,V_5) \cap \mathbb{P}(W) \cap Q0). There is no birational rigidity—every smooth GM threefold admits infinitely many non-isomorphic birational models within its period/double partner locus (Debarre et al., 2015).

For singular (specifically 1-nodal) GM threefolds, categorical resolutions of the Kuznetsov component, constructed via blowups and relating to Clifford modules over quadric fibrations, still detect the birational class of the original variety. A derived equivalence of these categorical resolutions implies the threefolds are birational (Grzelakowski et al., 15 Feb 2026).

Automorphism groups of GM threefolds are finite, with generic X=Gr(2,V5)∩P(W)∩QX = \mathrm{Gr}(2,V_5) \cap \mathbb{P}(W) \cap Q1 having only the identity or order-two involution (in the special case). An exception are highly symmetric examples, such as those with a faithful X=Gr(2,V5)∩P(W)∩QX = \mathrm{Gr}(2,V_5) \cap \mathbb{P}(W) \cap Q2-action studied in (Debarre et al., 2021). These symmetries have implications for the structure of X=Gr(2,V5)∩P(W)∩QX = \mathrm{Gr}(2,V_5) \cap \mathbb{P}(W) \cap Q3 and questions of rationality.

7. Moduli, K-Stability, and Deformation Theory

The moduli space of GM threefolds is irreducible of dimension 10, with the locus of special GM threefolds forming a divisor corresponding to degenerations of the associated EPW sextic (Liu et al., 2024). The K-moduli (moduli of K-stable varieties/log pairs) of special GM threefolds coincide with the moduli of log pairs X=Gr(2,V5)∩P(W)∩QX = \mathrm{Gr}(2,V_5) \cap \mathbb{P}(W) \cap Q4 with X=Gr(2,V5)∩P(W)∩QX = \mathrm{Gr}(2,V_5) \cap \mathbb{P}(W) \cap Q5 a quintic del Pezzo and X=Gr(2,V5)∩P(W)∩QX = \mathrm{Gr}(2,V_5) \cap \mathbb{P}(W) \cap Q6 an ordinary GM, with explicit walls given by values of X=Gr(2,V5)∩P(W)∩QX = \mathrm{Gr}(2,V_5) \cap \mathbb{P}(W) \cap Q7 (Liu et al., 2024).

All GM threefolds (ordinary and special) are K-stable; their moduli admit a chamber structure under varying the coefficient X=Gr(2,V5)∩P(W)∩QX = \mathrm{Gr}(2,V_5) \cap \mathbb{P}(W) \cap Q8 in the log pair, interpolating between ordinary and special loci. K-stability of special GM threefolds is reduced to the log K-stability of the pair X=Gr(2,V5)∩P(W)∩QX = \mathrm{Gr}(2,V_5) \cap \mathbb{P}(W) \cap Q9 (Liu et al., 2024).

Infinitesimal Torelli fails for ordinary GM threefolds (kernel of dimension 2), but holds for the invariant part of special GM threefolds via both Hodge-theoretic and categorical methods (Lin et al., 9 Jul 2025). The categorical viewpoint relates the kernel of the differential of the period map to moduli of stable objects in the Kuznetsov component, providing a geometric description of the non-Torelli directions.


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