Fano fourfolds of type A beta

zero loci on products of type A Grassmannians and flag varieties

Family 2-116-30-a

·

Blow-up of $\mathbb P^4$ along a surface.

  • $\varpi_1\colon X\to W$ is the blow-up of the del Pezzo fourfold $W$ of degree $5$, a linear section of $\mathrm{Gr}(2,5)$ (1-405-85-a), along a smooth rational surface of degree $11$, the blow-up of $\mathbb P^2$ in $10$ points.

  • $\varpi_3\colon X\to\mathbb P^4$ maps birationally onto $\mathbb P^4$ (1-625-126-a) with center a surface of degree $7$, smooth except at five non-normal points; the fibers are lines over the smooth points and quadric surfaces over the five special points.

Varieties in this family can be blown down to

Defining data
Ambient
Fl(1, 3, 5)
node 1: fundamental weight ω_1 (marked)node 2: fundamental weight ω_2node 3: fundamental weight ω_3 (marked)node 4: fundamental weight ω_4ω1ω2ω3ω4
Bundle
2 copies of E^(w3) + E^(w1 + w4)
Bundle
2 copies of O(0,1) + Q_1^v ot wedge^2 U_2^v ot Sym^2 U_3^v
ZL62 label
44.22U
Line bundles on the ambient $Y$
$$\begin{equation} \notag \begin{aligned} \omega_Y^\vee &\cong \mathcal{O}(3,4) \\ \det\mathcal{E} &\cong \mathcal{O}(2,3) \end{aligned} \end{equation}$$
Numerical invariants
Fano index = 1
$\mathrm{h}^0(X, \omega_X^\vee)$ = 30
$\operatorname{vol}(X) = \mathrm{c}_1^4$ = 116
$\chi(X, \mathrm{T}_X)$ = -14

$\omega_X^\vee \cong \mathcal{O}_X(1)$

Chern numbers of $\mathrm{T}_X$
$\mathrm{c}_1^4$ = 116
$\mathrm{c}_1^2\mathrm{c}_2$ = 116
$\mathrm{c}_2^2$ = 119
$\mathrm{c}_1\mathrm{c}_3$ = 34
$\mathrm{c}_4$ = 19
Hodge diamond
1
00
0 2 0
0 0 0 0
0 0 13 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 + 14 0 x0 + 14 x1
$\mathrm{HH}^{ 3 }$ = x1 + 26 0 0 x1 + 16 10
$\mathrm{HH}^{ 4 }$ = 30 0 0 0 0 30
$\mathrm{HH}^{ 5 }$ = 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

$\operatorname{Hilb}_X(t)$ $=$
$\displaystyle\frac{ 1 + 25t + 64t^{2} + 25t^{3} + t^{4} }{(1-t)^{ 5 }}$
$=$

Regularized quantum period

Quantum period in the literature

cataloguematching entries
Kalashnikov (2019) CKK(552)
Coates et al. (2020) No match
Coates–Kasprzyk–Prince (2015) No match

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) ^{2} \left( 3t + 1 \right) ^{3} \left( 944t^{5} + 736t^{4} + 1468t^{3} + 214t^{2} + 3t - 1 \right) \left( 144161840721920t^{15} + 507193720033280t^{14} + 849317289422848t^{13} + 870808865829888t^{12} + 589529480710144t^{11} + 269302369248512t^{10} + 83001236485312t^{9} + 17319466930944t^{8} + 2700388480672t^{7} + 454307010560t^{6} + 94527423824t^{5} + 15244773692t^{4} + 1365922586t^{3} + 48916459t^{2} - 90892t + 2987 \right)D^{6} + 2 \left( 2t + 1 \right) \left( 3t + 1 \right) ^{2} \left( 8573592991414026240t^{22} + 41162164104356986880t^{21} + 101911937663611977728t^{20} + 167096936131442999296t^{19} + 197909845494644121600t^{18} + 175832212037941168128t^{17} + 118773201567897953280t^{16} + 60992406738542179840t^{15} + 23667770439574811904t^{14} + 6920959076180204800t^{13} + 1559919678095029248t^{12} + 299751399117336160t^{11} + 59341401352130848t^{10} + 12498790217328864t^{9} + 2263821902371336t^{8} + 293154782386320t^{7} + 24531081060884t^{6} + 1265631068831t^{5} + 50565645969t^{4} + 2774154704t^{3} + 101130592t^{2} - 181143t + 2987 \right)D^{5} + \left( 3t + 1 \right) \left( 857359299141402624000t^{24} + 4604217063434767564800t^{23} + 12321161161871588065280t^{22} + 21498206433684934590464t^{21} + 27038393061216150749184t^{20} + 25718305989989181743104t^{19} + 18938254602901990203392t^{18} + 10894335703885451350016t^{17} + 4899861078549453244416t^{16} + 1720697124927521897984t^{15} + 475219837855099783680t^{14} + 107525132725997280896t^{13} + 22279960879660706496t^{12} + 4822170577652471936t^{11} + 1052338182759507616t^{10} + 195357052224093280t^{9} + 27057737127554152t^{8} + 2575103269545464t^{7} + 153524557160016t^{6} + 4593195795491t^{5} - 15297675759t^{4} - 6219823690t^{3} - 204401902t^{2} - 101569t - 2987 \right)D^{4} + 2 t \left( 5401363584590836531200t^{24} + 29686018151223086284800t^{23} + 80346608658124093194240t^{22} + 140646130698158656962560t^{21} + 176576881168844311445504t^{20} + 167312114262317372788736t^{19} + 122920894783898075369472t^{18} + 70952778938779039522816t^{17} + 32340009588354905909248t^{16} + 11667806570394052415744t^{15} + 3365692734146087894784t^{14} + 808149672503027512128t^{13} + 178722870560850708704t^{12} + 41005911773883055840t^{11} + 9554967649838448560t^{10} + 1950840007732880616t^{9} + 309005884914716688t^{8} + 35324803578579286t^{7} + 2737077810201953t^{6} + 130999224132580t^{5} + 3222635627439t^{4} + 28100752266t^{3} + 550082755t^{2} + 9561572t + 2781 \right)D^{3} + 4 t ^{2} \left( 5967220722024162263040t^{23} + 31848466776118891315200t^{22} + 83247536610832247586816t^{21} + 139885086600087024893952t^{20} + 167429269388209280032768t^{19} + 150135993029373503868928t^{18} + 103643308316583974629376t^{17} + 55862152736988673527808t^{16} + 23663273297123318060544t^{15} + 7925158720055825276928t^{14} + 2142116321046932356352t^{13} + 499929830313686767488t^{12} + 115195313956713317472t^{11} + 28462604779803933552t^{10} + 6790959689067746056t^{9} + 1337779961898817532t^{8} + 197895257434633754t^{7} + 20749113302236036t^{6} + 1449942679334996t^{5} + 61094070118865t^{4} + 1284291592217t^{3} + 12433565657t^{2} + 403673877t + 3261282 \right)D^{2} + 4 t ^{2} \left( 6481636301509003837440t^{23} + 33839806523219916226560t^{22} + 86228588613302533029888t^{21} + 140640517987700535754752t^{20} + 162470792297646842888192t^{19} + 139673075387848567848960t^{18} + 91779954914764952248320t^{17} + 46768505876316514973696t^{16} + 18630333011706748136448t^{15} + 5861740252950169488896t^{14} + 1506826910060182354432t^{13} + 349018838165173917184t^{12} + 84751007138226779200t^{11} + 22048715319296458400t^{10} + 5248063539711200272t^{9} + 990966100751751848t^{8} + 137812182370272564t^{7} + 13419658101037712t^{6} + 858982069487812t^{5} + 32464435193222t^{4} + 603950338593t^{3} + 7198794788t^{2} + 229719045t + 1147008 \right)D + 16 t ^{2} \left( 661391459337653452800t^{23} + 3401046868018131763200t^{22} + 8517823326598363545600t^{21} + 13613815382458678345728t^{20} + 15345519576073102917632t^{19} + 12802152733601411473408t^{18} + 8112794723434125381632t^{17} + 3961357081949374151680t^{16} + 1503851734295088986112t^{15} + 450358366787226498560t^{14} + 111612831939607130368t^{13} + 25989720552183962432t^{12} + 6626580413918078432t^{11} + 1777177333774574464t^{10} + 417417224078505904t^{9} + 75801945363214704t^{8} + 10013013296373832t^{7} + 917744134874218t^{6} + 54662643226483t^{5} + 1891192423996t^{4} + 32630083537t^{3} + 507405246t^{2} + 12703814t + 41818 \right) \notag \end{equation}$$

Quantum spectrum

Ambient: Fl(1, 3, 5)

|λ| = 18.72989 λ ≈ 18.72989; multiplicity 1; Jordan blocks 1 λ ≈ -7.650441 - 3.852102i; multiplicity 1; Jordan blocks 1 λ ≈ -7.650441 + 3.852102i; multiplicity 1; Jordan blocks 1 λ ≈ -3; multiplicity 3; Jordan blocks 1, 2 λ ≈ -2; multiplicity 2; Jordan blocks 2 λ ≈ -0.2145033 - 0.8005915i; multiplicity 1; Jordan blocks 1 λ ≈ -0.2145033 + 0.8005915i; multiplicity 1; Jordan blocks 1 3 2
Sector dimension
10
Spectral radius
$18.7298891$
Diagonalizable at 1
No
Simple spectrum at 1
No
Eigenvalue approximations and Jordan block sizes
eigenvaluemultiplicityJordan blocks
$18.72989$11
$-7.650441 - 3.852102\mathrm{i}$11
$-7.650441 + 3.852102\mathrm{i}$11
$-3$31, 2
$-2$22
$-0.2145033 - 0.8005915\mathrm{i}$11
$-0.2145033 + 0.8005915\mathrm{i}$11

Characteristic polynomial

$$\begin{equation}\left(\lambda + 2\right)^{2} \left(\lambda + 3\right)^{3} \left(\lambda^{5} - 3 \lambda^{4} - 214 \lambda^{3} - 1468 \lambda^{2} - 736 \lambda - 944\right)\notag\end{equation}$$

Minimal polynomial

$$\begin{equation}\left(\lambda + 2\right)^{2} \left(\lambda + 3\right)^{2} \left(\lambda^{5} - 3 \lambda^{4} - 214 \lambda^{3} - 1468 \lambda^{2} - 736 \lambda - 944\right)\notag\end{equation}$$

Quantum multiplication matrix

$$\begin{equation}\begin{pmatrix}0 & 14 & 14 & 96 & 54 & 60 & 42 & 80 & 224 & 300 \\ 1 & -1 & 4 & 12 & 10 & 4 & 2 & 18 & 48 & 48 \\ 1 & 2 & -1 & 26 & 16 & 14 & 10 & 18 & 48 & 64 \\ 0 & 1 & 1 & -2 & 0 & 2 & 2 & 2 & 8 & 12 \\ 0 & 1 & 0 & 4 & -1 & 2 & 1 & 0 & 0 & 6 \\ 0 & 0 & 1 & 2 & 1 & -2 & -1 & 4 & 8 & 6 \\ 0 & 0 & 1 & 2 & 3 & 0 & -1 & 2 & 8 & 6 \\ 0 & 0 & 0 & -6 & -8 & 2 & 2 & -7 & -8 & 0 \\ 0 & 0 & 0 & \frac{25}{4} & \frac{21}{4} & \frac{7}{4} & 1 & \frac{7}{2} & 5 & 7 \\ 0 & 0 & 0 & 0 & 0 & 0 & 0 & \frac{3}{2} & 4 & 0\end{pmatrix}\notag\end{equation}$$