# Algebraic Geometry Seminar Spring 2017: Difference between revisions

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Schur-Weyl duality is an important result in representation theory which states that the actions of <math>\mathfrak{S}_n</math> and <math>\mathbf{GL}(N)</math> on <math>\mathbf{V}^{\otimes n}</math> generate each others' commutants. Here <math>\mathfrak{S}_n</math> is the symmetric group and <math>\mathbf{V}</math> is the standard complex representation. In this talk, we investigate the Spin-Brauer diagram algebra, which arises from studying an analogous form of Schur-Weyl duality for the action of the spinor group on <math>\mathbf{V}^{\otimes n} \otimes \Delta</math>. Here <math>\mathbf{V}</math> is again the standard <math>N</math>-dimensional complex representation of <math>{\rm Pin}(N)</math> and <math>\Delta</math> is the spin representation. We will give a general construction of the Spin-Brauer diagram algebra, discuss its connection to <math>{\rm End}_{{\rm Pin}(N)}(V^{\otimes n} \otimes \Delta)</math> and time permitting we will mention some interesting properties of the algebra, in particular its cellularity. | Schur-Weyl duality is an important result in representation theory which states that the actions of <math>\mathfrak{S}_n</math> and <math>\mathbf{GL}(N)</math> on <math>\mathbf{V}^{\otimes n}</math> generate each others' commutants. Here <math>\mathfrak{S}_n</math> is the symmetric group and <math>\mathbf{V}</math> is the standard complex representation. In this talk, we investigate the Spin-Brauer diagram algebra, which arises from studying an analogous form of Schur-Weyl duality for the action of the spinor group on <math>\mathbf{V}^{\otimes n} \otimes \Delta</math>. Here <math>\mathbf{V}</math> is again the standard <math>N</math>-dimensional complex representation of <math>{\rm Pin}(N)</math> and <math>\Delta</math> is the spin representation. We will give a general construction of the Spin-Brauer diagram algebra, discuss its connection to <math>{\rm End}_{{\rm Pin}(N)}(V^{\otimes n} \otimes \Delta)</math> and time permitting we will mention some interesting properties of the algebra, in particular its cellularity. | ||

===Nathan Clement=== | |||

'''Parabolic Higgs bundles and the Poincare line bundle''' |

## Revision as of 23:33, 21 February 2017

The seminar meets on Fridays at 2:25 pm in Van Vleck B113.

Here is the schedule for the previous semester.

## Algebraic Geometry Mailing List

- Please join the AGS Mailing List to hear about upcoming seminars, lunches, and other algebraic geometry events in the department (it is possible you must be on a math department computer to use this link).

## Spring 2017 Schedule

date | speaker | title | host(s) |
---|---|---|---|

January 20 | Sam Raskin (MIT) | W-algebras and Whittaker categories | Dima |

January 27 | Nick Salter (U Chicago) | Mapping class groups and the monodromy of some families of algebraic curves | Jordan |

March 3 | Robert Laudone (UW Madison) | The Spin-Brauer diagram algebra | local (Steven) |

March 10 | Nathan Clement (UW Madison) | Parabolic Higgs bundles and the Poincare line bundle | local |

March 17 | Amy Huang (UW Madison) | TBA | local (Steven) |

March 31 | Jie Zhou (Perimeter Institute) | TBA | Andrei |

April 7 | Vladimir Dokchitser (Warwick) | TBA | Jordan |

## Abstracts

### Sam Raskin

**W-algebras and Whittaker categories**

Affine W-algebras are a somewhat complicated family of (topological) associative algebras associated with a semisimple Lie algebra, quantizing functions on the algebraic loop space of Kostant's slice. They have attracted a great deal of attention because of Feigin-Frenkel's duality theorem for them, which identifies W-algebras for a Lie algebra and for its Langlands dual through a subtle construction.

The purpose of this talk is threefold: 1) to introduce a ``stratification" of the category of modules for the affine W-algebra, 2) to prove an analogue of Skryabin's equivalence in this setting, realizing the categoryof (discrete) modules over the W-algebra in a more natural way, and 3) to explain how these constructions help understand Whittaker categories in the more general setting of local geometric Langlands. These three points all rest on the same geometric observation, which provides a family of affine analogues of Bezrukavnikov-Braverman-Mirkovic. These results lead to a new understanding of the exactness properties of the quantum Drinfeld-Sokolov functor.

### Nick Salter

**Mapping class groups and the monodromy of some families of algebraic curves**

In this talk we will be concerned with some topological questions arising in the study of families of smooth complex algebraic curves. Associated to any such family is a monodromy representation valued in the mapping class group of the underlying topological surface. The induced action on the cohomology of the fiber has been studied for decades- the more refined topological monodromy is largely unexplored. In this talk, I will discuss some theorems concerning the topological monodromy groups of families of smooth plane curves, as well as families of curves in CP^1 x CP^1. This will involve a blend of algebraic geometry, singularity theory, and the mapping class group, particularly the Torelli subgroup.

### Robert Laudone

**The Spin-Brauer diagram algebra**

Schur-Weyl duality is an important result in representation theory which states that the actions of [math]\displaystyle{ \mathfrak{S}_n }[/math] and [math]\displaystyle{ \mathbf{GL}(N) }[/math] on [math]\displaystyle{ \mathbf{V}^{\otimes n} }[/math] generate each others' commutants. Here [math]\displaystyle{ \mathfrak{S}_n }[/math] is the symmetric group and [math]\displaystyle{ \mathbf{V} }[/math] is the standard complex representation. In this talk, we investigate the Spin-Brauer diagram algebra, which arises from studying an analogous form of Schur-Weyl duality for the action of the spinor group on [math]\displaystyle{ \mathbf{V}^{\otimes n} \otimes \Delta }[/math]. Here [math]\displaystyle{ \mathbf{V} }[/math] is again the standard [math]\displaystyle{ N }[/math]-dimensional complex representation of [math]\displaystyle{ {\rm Pin}(N) }[/math] and [math]\displaystyle{ \Delta }[/math] is the spin representation. We will give a general construction of the Spin-Brauer diagram algebra, discuss its connection to [math]\displaystyle{ {\rm End}_{{\rm Pin}(N)}(V^{\otimes n} \otimes \Delta) }[/math] and time permitting we will mention some interesting properties of the algebra, in particular its cellularity.

### Nathan Clement

**Parabolic Higgs bundles and the Poincare line bundle**