On the period map for prime Fano threefolds of degree 10
By O. Debarre, A. Iliev, Laurent Manivel. 2008
51 citations recorded by the source corpus.
We prove that the deformations of a smooth complex Fano threefold X with Picard number 1, index 1, and degree 10, are unobstructed. The differential of the period map has two-dimensional kernel. We construct two two-dimensional components of the fiber of the period map through X: one is isomorphic to the variety of conics in X, modulo an involution, another is birationally isomorphic to a moduli space of semistable rank-2 torsion-free sheaves on X, modulo an involution. The threefolds corresponding to points of these components are obtained from X via conic and line (birational) transformations.
Subfields: Geometry and Topology, Mathematical Physics
View Paper: https://www.semanticscholar.org/paper/eef18a1182aa187ff1112dcb5b6d6f26cdfa284a
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In Geometry and Topology
- Alexander Perry
- Alexander Kuznetsov
- O. Debarre
- Laurent Manivel
- Emanuele Macrì
- P. Stellari
- K. Hori
- Daniele Faenzi
In Mathematical Physics
- Alexander Perry
- Alexander Kuznetsov
- O. Debarre
- Laurent Manivel
- K. Hori
- Emanuele Macrì
- P. Stellari
- I. Smith
Citations in the corpus
- Gushel--Mukai varieties: classification and birationalities (2015, background): “phic (Theorem 4.20). The birational isomorphisms relating periodpartners are generalizations ofconic transformations and those relating dual varieties are generalizations of line transformations (see [DIM]). In relation with birationalities for dual varieties, we define another interesting geometric ”
- The integral Hodge conjecture for two-dimensional Calabi–Yau categories (2020, background): “Recently, GM varieties have attracted attention because of the rich structure of their birational geometry, Hodge theory, and derived categories [22, 42, 23, 25, 26, 27, 57, 76].”
- Special prime Fano fourfolds of degree 10 and index 2 (2013, background): “NO FOURFOLDS 7 As in the first case above, the kernel K is therefore isomorphic to H1(PW,Ω3 PW ⊗OPW(2)). Using (6) again, we obtain an exact sequence H1(W,Ω3 W ⊗ Sym 2 E) → K → H1(W,Ω2 W ⊗ det(E)). By [DIM1], Proposition 5.3, we have H1(W,Ω3 W ⊗ Sym 2 E) = H1(W,Ω3 W(2)) ≃ H3(W,Ω1 W(−2))∨, H1(W,Ω2 W ⊗”