Fano fourfolds of type A beta

zero loci on products of type A Grassmannians and flag varieties

Family 2-256-57-b

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No geometric description is recorded for this family (yet).

Defining data
Ambient
Fl(2, 4, 8)
node 1: fundamental weight ω_1node 2: fundamental weight ω_2 (marked)node 3: fundamental weight ω_3node 4: fundamental weight ω_4 (marked)node 5: fundamental weight ω_5node 6: fundamental weight ω_6node 7: fundamental weight ω_7ω1ω2ω3ω4ω5ω6ω7
Bundle
3 copies of E^(w7) + E^(2w1) + E^(2w4)
Bundle
3 copies of wedge^3 Q_1^v ot wedge^2 U_2^v ot wedge^2 U_3^v + Sym^2 U_3^v + O(0,2)
ZL62 label
709.666A7
Line bundles on the ambient $Y$
$$\begin{equation} \notag \begin{aligned} \omega_Y^\vee &\cong \mathcal{O}(4,6) \\ \det\mathcal{E} &\cong \mathcal{O}(3,5) \end{aligned} \end{equation}$$
Numerical invariants
Fano index = 2
$\mathrm{h}^0(X, \omega_X^\vee)$ = 57
$\operatorname{vol}(X) = \mathrm{c}_1^4$ = 256
$\chi(X, \mathrm{T}_X)$ = 0

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

Chern numbers of $\mathrm{T}_X$
$\mathrm{c}_1^4$ = 256
$\mathrm{c}_1^2\mathrm{c}_2$ = 160
$\mathrm{c}_2^2$ = 96
$\mathrm{c}_1\mathrm{c}_3$ = 48
$\mathrm{c}_4$ = 0
Hodge diamond
1
00
0 2 0
0 2 2 0
0 0 2 0 0
0 2 2 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 + x2 0 x0 x2
$\mathrm{HH}^{ 3 }$ = x1 + 64 0 0 x1 64
$\mathrm{HH}^{ 4 }$ = x1 - x2 + 63 0 0 x1 - x2 + 6 0 57
$\mathrm{HH}^{ 5 }$ = 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

$\operatorname{Hilb}_X(t)$ $=$
$\displaystyle\frac{ 1 + 7t + 7t^{2} + t^{3} }{(1-t)^{ 5 }}$
$=$

Regularized quantum period

Quantum period in the literature

cataloguematching entries
Kalashnikov (2019) CKK(442)
Coates et al. (2020) P1 x B(3,4)
Coates–Kasprzyk–Prince (2015) CKP(500)

Quantum differential equation

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

$$\begin{equation} L_X=\left( 6t - 1 \right) \left( 6t + 1 \right) \left( 10t - 1 \right) \left( 10t + 1 \right) \left( 2t - 1 \right) ^{2} \left( 2t + 1 \right) ^{2} \left( 1433040t^{6} + 80728t^{4} - 2579t^{2} + 1 \right)D^{6} + 2 \left( 2t - 1 \right) \left( 2t + 1 \right) \left( 226993536000t^{12} - 6984049920t^{10} - 2174297216t^{8} + 67707232t^{6} - 106452t^{4} - 7441t^{2} + 2 \right)D^{5} + 4 \left( 3920797440000t^{14} - 584516290560t^{12} - 52264472064t^{10} + 4812821760t^{8} - 86750536t^{6} + 175464t^{4} - 4911t^{2} + 1 \right)D^{4} + 8 t ^{2} \left( 8460668160000t^{12} - 550314631680t^{10} - 112753881472t^{8} + 5245181728t^{6} - 97715360t^{4} - 329920t^{2} - 69 \right)D^{3} + 32 t ^{2} \left( 4769443728000t^{12} - 59034734400t^{10} - 53369502424t^{8} + 1881440232t^{6} - 26802560t^{4} - 94678t^{2} - 5 \right)D^{2} + 768 t ^{4} \left( 219040164000t^{10} + 4402781840t^{8} - 2035415446t^{6} + 67181120t^{4} - 620103t^{2} - 1737 \right)D + 4608 t ^{4} \left( 15046920000t^{10} + 593723200t^{8} - 120630700t^{6} + 4065994t^{4} - 22137t^{2} - 34 \right) \notag \end{equation}$$

Quantum spectrum

Ambient: Fl(2, 4, 8)

|λ| = 10 λ ≈ -10; multiplicity 1; Jordan blocks 1 λ ≈ 10; multiplicity 1; Jordan blocks 1 λ ≈ -6; multiplicity 1; Jordan blocks 1 λ ≈ 6; multiplicity 1; Jordan blocks 1 λ ≈ -2; multiplicity 2; Jordan blocks 2 λ ≈ 2; multiplicity 2; Jordan blocks 2 2 2
Sector dimension
8
Spectral radius
$10$
Diagonalizable at 1
No
Simple spectrum at 1
No
Eigenvalue approximations and Jordan block sizes
eigenvaluemultiplicityJordan blocks
$-10$11
$10$11
$-6$11
$6$11
$-2$22
$2$22

Characteristic polynomial

$$\begin{equation}\left(\lambda + 2\right)^{2} \left(\lambda + 6\right) \left(\lambda + 10\right) \left(\lambda - 10\right) \left(\lambda - 2\right)^{2} \left(\lambda - 6\right)\notag\end{equation}$$

Minimal polynomial

$$\begin{equation}\left(\lambda + 2\right)^{2} \left(\lambda + 6\right) \left(\lambda + 10\right) \left(\lambda - 10\right) \left(\lambda - 2\right)^{2} \left(\lambda - 6\right)\notag\end{equation}$$

Quantum multiplication matrix

$$\begin{equation}\begin{pmatrix}0 & 12 & 8 & 0 & 0 & 0 & 32 & 0 \\ 1 & 0 & 0 & 8 & 8 & 0 & 0 & 32 \\ 1 & 0 & 0 & -4 & 12 & 0 & 0 & -32 \\ 0 & 1 & -1 & 0 & 0 & 12 & 4 & 0 \\ 0 & 2 & 2 & 0 & 0 & 4 & 12 & 0 \\ 0 & 0 & 0 & 2 & 1 & 0 & 0 & 4 \\ 0 & 0 & 0 & 0 & 2 & 0 & 0 & 4 \\ 0 & 0 & 0 & 0 & 0 & 2 & 3 & 0\end{pmatrix}\notag\end{equation}$$