Fano fourfolds of type A beta

zero loci on products of type A Grassmannians and flag varieties

Family 2-480-99-a

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The projective bundle $\mathbb P_{Q^3}(\mathcal O\oplus\mathcal O(-1))$ over a smooth quadric threefold.

  • $\pi_1\colon X\to Q^3$ is the $\mathbb P^1$-bundle $\mathbb P_{Q^3}(\mathcal O\oplus\mathcal O(-1))$ over a smooth quadric threefold.

  • $\pi_2\colon X\to\mathbb P^5\times\mathbb P^4$ is an isomorphism onto its image.

  • $\pi_3\colon X\to\mathbb P^5\times\mathrm{Gr}(2,6)$ is an isomorphism onto its image.

  • $\pi_{23}\colon X\to C$ is the blow-up of the vertex of a quadric cone $C\subset\mathbb P^5$ of corank one (the cone over a smooth quadric threefold); the exceptional divisor is a quadric threefold with normal bundle $\mathcal O(-1)$.

Varieties in this family can be blown down to

  • A quadric cone in $\mathbb P^5$ of corank one
Defining data
Ambient
Fl(1, 2, 6) × ℙ4P4
node 1: fundamental weight ω_1 (marked)node 2: fundamental weight ω_2 (marked)node 3: fundamental weight ω_3node 4: fundamental weight ω_4node 5: fundamental weight ω_5node 6: fundamental weight ω_6 (marked)node 7: fundamental weight ω_7node 8: fundamental weight ω_8node 9: fundamental weight ω_9ω1ω2ω3ω4ω5ω6ω7ω8ω9
Bundle
E^(w5) + E^(w5 + w6) + E^(2w2)
Bundle
wedge^3 Q_1,1^v ot U_1,2^v ot U_1,3^v + wedge^3 Q_1,1^v ot U_1,2^v ot U_1,3^v box O_2(1) + O_1(0,2)
ZL62 label
4052.8Ew7
Line bundles on the ambient $Y$
$$\begin{equation} \notag \begin{aligned} \omega_Y^\vee &\cong \mathcal{O}(2,5;5) \\ \det\mathcal{E} &\cong \mathcal{O}(0,4;4) \end{aligned} \end{equation}$$
Numerical invariants
Fano index = 2
$\mathrm{h}^0(X, \omega_X^\vee)$ = 99
$\operatorname{vol}(X) = \mathrm{c}_1^4$ = 480
$\chi(X, \mathrm{T}_X)$ = 16

$\omega_X^\vee \cong \mathcal{O}_X(2)$

Chern numbers of $\mathrm{T}_X$
$\mathrm{c}_1^4$ = 480
$\mathrm{c}_1^2\mathrm{c}_2$ = 216
$\mathrm{c}_2^2$ = 96
$\mathrm{c}_1\mathrm{c}_3$ = 56
$\mathrm{c}_4$ = 8
Hodge diamond
1
00
0 2 0
0 0 0 0
0 0 2 0 0
0 0 0 0
0 2 0
00
1
Polyvector parallelogram & Hochschild cohomology
$\mathrm{HH}^{ 0 }$ = 1 1
$\mathrm{HH}^{ 1 }$ = x0 0 x0
$\mathrm{HH}^{ 2 }$ = x0 + x1 - 16 0 x0 - 16 x1
$\mathrm{HH}^{ 3 }$ = x1 + 76 0 0 x1 - 80 156
$\mathrm{HH}^{ 4 }$ = 99 0 0 0 0 99
$\mathrm{HH}^{ 5 }$ = 0 0 0 0 0
$\mathrm{HH}^{ 6 }$ = 0 0 0 0
$\mathrm{HH}^{ 7 }$ = 0 0 0
$\mathrm{HH}^{ 8 }$ = 0 0

Hilbert series

$\operatorname{Hilb}_X(t)$ $=$
$\displaystyle\frac{ 1 + 14t + 14t^{2} + t^{3} }{(1-t)^{ 5 }}$
$=$

Regularized quantum period

Quantum period in the literature

cataloguematching entries
Kalashnikov (2019) CKK(39)
Coates et al. (2020) MW(13)
Coates–Kasprzyk–Prince (2015) CKP(60)

Quantum differential equation

With $D=t\frac{\mathrm{d}}{\mathrm{d}t}$, the regularized period satisfies $L_X\widehat{\mathrm{G}}_X=0$.

$$\begin{equation} L_X=\left( 2t - 1 \right) \left( 2t + 1 \right) \left( 136t^{3} - 20t^{2} + 6t - 1 \right) \left( 136t^{3} + 20t^{2} + 6t + 1 \right) \left( 66683996t^{6} - 1058780t^{4} - 19394t^{2} + 15 \right)D^{6} + 4 \left( 27134518180352t^{14} - 3636686279168t^{12} - 76696829376t^{10} + 3834603264t^{8} - 107218310t^{6} + 2061400t^{4} + 29091t^{2} - 15 \right)D^{5} + 4 \left( 234343566103040t^{14} - 21804386465792t^{12} + 102596245216t^{10} + 15956069184t^{8} + 542705432t^{6} - 1694520t^{4} - 36762t^{2} + 15 \right)D^{4} + 32 t ^{2} \left( 126422186976640t^{12} - 8667906294144t^{10} + 129634375864t^{8} + 2690207848t^{6} + 17651600t^{4} - 204240t^{2} - 49 \right)D^{3} + 32 t ^{2} \left( 285066614292448t^{12} - 15534154687040t^{10} + 251203935368t^{8} - 291393828t^{6} - 1136928t^{4} - 258660t^{2} - 15 \right)D^{2} + 128 t ^{4} \left( 78551346664144t^{10} - 3663416463632t^{8} + 48257529676t^{6} - 820898270t^{4} - 4423658t^{2} - 37545 \right)D + 3072 t ^{4} \left( 1349017239080t^{10} - 57143052340t^{8} + 533807468t^{6} - 19445050t^{4} - 103234t^{2} - 345 \right) \notag \end{equation}$$

Quantum spectrum

Ambient: Fl(1, 2, 6) × ℙ4P4

|λ| = 6.269769 λ ≈ -6.269769; multiplicity 1; Jordan blocks 1 λ ≈ 6.269769; multiplicity 1; Jordan blocks 1 λ ≈ -0.1348845 - 4.655448i; multiplicity 1; Jordan blocks 1 λ ≈ -0.1348845 + 4.655448i; multiplicity 1; Jordan blocks 1 λ ≈ 0.1348845 - 4.655448i; multiplicity 1; Jordan blocks 1 λ ≈ 0.1348845 + 4.655448i; multiplicity 1; Jordan blocks 1 λ ≈ -2; multiplicity 1; Jordan blocks 1 λ ≈ 2; multiplicity 1; Jordan blocks 1
Sector dimension
8
Spectral radius
$6.269769$
Diagonalizable at 1
Yes
Simple spectrum at 1
Yes
Eigenvalue approximations and Jordan block sizes
eigenvaluemultiplicityJordan blocks
$-6.269769$11
$6.269769$11
$-0.1348845 - 4.655448\mathrm{i}$11
$-0.1348845 + 4.655448\mathrm{i}$11
$0.1348845 - 4.655448\mathrm{i}$11
$0.1348845 + 4.655448\mathrm{i}$11
$-2$11
$2$11

Characteristic polynomial

$$\begin{equation}\left(\lambda + 2\right) \left(\lambda - 2\right) \left(\lambda^{3} + 6 \lambda^{2} + 20 \lambda + 136\right) \left(\lambda^{3} - 6 \lambda^{2} + 20 \lambda - 136\right)\notag\end{equation}$$

Minimal polynomial

$$\begin{equation}\left(\lambda + 2\right) \left(\lambda - 2\right) \left(\lambda^{3} + 6 \lambda^{2} + 20 \lambda + 136\right) \left(\lambda^{3} - 6 \lambda^{2} + 20 \lambda - 136\right)\notag\end{equation}$$

Quantum multiplication matrix

$$\begin{equation}\begin{pmatrix}0 & 2 & 0 & 0 & 0 & 8 & 0 & 0 \\ 2 & 0 & 0 & 0 & 4 & 0 & 0 & 0 \\ 2 & 0 & 0 & 2 & -4 & 0 & 0 & 8 \\ 0 & 4 & 2 & 0 & 0 & 0 & 4 & 0 \\ 0 & 0 & 2 & 0 & 0 & 2 & -4 & 0 \\ 0 & 0 & 0 & 4 & 2 & 0 & 0 & 0 \\ 0 & 0 & 0 & 0 & 2 & 0 & 0 & 2 \\ 0 & 0 & 0 & 0 & 0 & 4 & 2 & 0\end{pmatrix}\notag\end{equation}$$