## Quantum Lefshetz for non-split bundle via “abelian/non-abelian correspondence”.

Bumsig Kim explained me how their beautiful theory provides a tool for computing J-series of and many other Fano threefolds.

The computation for can be reproduced by the following pari/gp code (I omit checking that mirror map is almost trivial):

N=9

o = O(t^(N+1))

h(n) = sum(k=1,n,1/k)

hh(n) = sum(k=1,n,sum(l=k+1,n,1/k/l))

gg(x, p) = (x!*(1+h(x)*p+hh(x)*p^2+O(u^4)))

simplemirrormap(F) = F * exp(-polcoeff(F,1,t)*t)

reg(F) = sum(n=0,N,t^n*polcoeff(F,n,t)*n!)+O(t^(N+1))

period(F) = reg(simplemirrormap(F))

```
```gp > v22 = period( polcoeff( sum(a=0,N,sum(b=0,N,sum(c=0,N,o+ t^(a+b+c)* ( gg(a+b,u*(A+B)) * gg(a+c,u*(A+C)) * gg(b+c,u*(B+C)) )^3 / (gg(a,u*A) * gg(b,u*B) * gg(c,u*C) )^7 *(c-b+u*(C-B))*(c-a+u*(C-A))*(b-a+u*(B-A)) ))) + O(u^4) , 3,u) /(C-B)/(C-A)/(B-A) + o )

`%2 = 1 + 12*t^2 + 60*t^3 + 636*t^4 + 5760*t^5 + 58620*t^6 + 604800*t^7 + 6447420*t^8 + O(t^9)`

Indeed, period sequence 17.

Note that is the familiar Gamma-factor with .

——————————————————-

So, how does it works?

Consider 3-dimensional vector space with a fixed base, 7-dimensional vector space , and space of 3×7 matrices

Group acts on M by left multiplication. It has a subgroup of diagonal matrices and one may restrict the action to this smaller subgroup.

Let be the subset of matrices of maximal rank and be the subset of matrices with non-vanishing rows, is an open subset in .

Consider quotient spaces and . Note that and .

Since T is a subgroup of G, there is a natural rational map : a triple of points in is sent to their linear span.

Weyl group (symmetric group ) acts on and hence it acts on the cohomology , so cohomology space is decomposed into representations of .

[I’ll omit the part of the story with the partial flag space and non-holomorphic map].

**1.** It turns out that cohomology can be identified with antisymmetric part of as a graded vector space (with grading shifted by 3).

Explicitly, is generated by 3 pullbacks of hyperplane sections on ; cohomologies of Grassmanian are known to be quotient of symmetric polynomials. Vector space of anti-symmetric polynomials is obtained from vector space of symmetric polynomials via multiplication by anti-symmetric polynomial of the smallest degree and by pulling them back to M, and considering as G-linearized.

It turns out that universal bundle U over Gr(3,7) decomposes into sum of 3 line bundles on .

So and .

**3.** On domain of one may define a relative tangent bundle (“traceless” part of ). It turns out this vector bundle can be extended as a split vector bundle to whole : .

Consider “square root” of relative tangent bundle .

**4.**Recall that Fano threefolds are sections of homogeneous vector bundle on . Comparision (2) shows these threefolds has 9-dimensional abelianizations — complete intersections of $9$-dimensional split bundle on .

**5.** Abelian/non-abelian correspondence is similar for pairs and .

J-series for Gr(3,7) can be obtained as twisted by relative tangent bundle I-series for after the comparision of cohomologies described in (1).

Similarly, J-series for can be obtained via mirror map from twisted by I-series after the “pullbacked” comparision (1).

**6.** The sign comes from considering closely the Gamma-factor for relative tangent bundle . Note that fibers of abelian/non-abelian correspondence are in some sense holomorphic symplectic (relative tangent bundle contains both O(D) and O(-D)), so they behave like varieties with trivial canonical class.

Consider the factor . Since and we have .

The same method can also be applied to complete intersections of homogeneous bundles in orthogonal isotropic and symplectic isotropic Grassmanians, since these Grassmanians themselves are just sections of some homogeneous bundles (wedge or symmetric powers of universal bundle) on ordinary Grassmanians of type A. Also this can be uprgaded to treat different blowups of these varieties. In particular, in the comments to this post I compute J-series for Fano threefolds **, #2.14, #2.17, #2.20, #2.21 and #2.22**.

Also Bumsig points out that one can express the ab/non-ab twist as a differential operator applied to abelian multi-parameter J-function (basically, just Vandermonde . This interpretation is more useful for dealing with Frobenius manifolds.

References:

Gromov-Witten Invariants for Abelian and Nonabelian Quotients by Aaron Bertram, Ionut Ciocan-Fontanine, Bumsig Kim

The Abelian/Nonabelian Correspondence and Frobenius Manifolds by Ionut Ciocan-Fontanine, Bumsig Kim, Claude Sabbah

Quantum cohomology of the Grassmannian and alternate Thom-Sebastiani by Bumsig Kim, Claude Sabbah