Fanography

A tool to visually study the geography of Fano 3-folds.

Identification

Fano variety 2-2

double cover of 2-34 with branch locus a $(2,4)$-divisor

Picard rank
2 (others)
$-\mathrm{K}_X^3$
6
$\mathrm{h}^{1,2}(X)$
20
Mori–Mukai $d$
-4
Hodge diamond and polyvector parallelogram
1
0 0
0 2 0
0 20 20 0
0 2 0
0 0
1
1
0 0
0 33 0
0 0 0 6
0 6 0
0 0
0
Poisson structures

Still open.

Anticanonical bundle
index
1
$\dim\mathrm{H}^0(X,\omega_X^\vee)$
6
$-\mathrm{K}_X$ very ample?
no
$-\mathrm{K}_X$ basepoint free?
yes
hyperelliptic
yes
trigonal
no
Birational geometry

This variety is not rational but unirational.

A very general member is not stably rational.

The Weyl group associated to the KKMR decomposition is $\mathrm{A}_1$; see the Weyl-group table for sources and conventions.


This variety is primitive.

Deformation theory
number of moduli
33
Bott vanishing
does not hold
$\mathrm{Aut}^0(X)$$\dim\mathrm{Aut}^0(X)$number of moduli
$0$033
Period sequence

There is no period sequence associated to this Fano 3-fold.

Extremal contractions
Semiorthogonal decompositions

There exist interesting semiorthogonal decompositions, but this data is not yet added.

Structure of quantum cohomology

By Hertling–Manin–Teleman we have that quantum cohomology cannot be generically semisimple, as $\mathrm{h}^{1,2}\neq 0$.

Zero section description

Fano 3-folds from homogeneous vector bundles over Grassmannians gives the following description(s):

variety
$\mathbb{P}^1\times \mathbb{P}^2 \times \mathbb{P}^{12}$
bundle
$\mathcal{O}(0,0,2) \oplus K(0,0,1)$

See the big table for more information.

K-stability
  • every member is K‑stable
  • every member is K‑polystable
  • every member is K‑semistable
Seeand the big table for more information.
Coregularity

For this deformation family, every smooth member has coregularity 0.

The generic and uniform statements are due to Avilov–Loginov–Przyjalkowski; the existence of a smooth member of coregularity zero in every family is due to Zhakupov.

See coregularity for terminology.

Futaki invariant

For every K-polystable member, the Futaki invariant vanishes identically on the entire Kähler cone.

This is the computation of Sektnan–Tipler.