Learning Seminar on Conformal Field Theory (Fall 2019)
The goal of this seminar is to understand various aspects of conformal field theory from a mathematical perspective.
 Organizer: Henry Liu
 Time/date: Tuesdays 1:102:25pm
 Location: Math 622
I am liveTeXing notes for this seminar, available here.
Please email me at hliu at math dot columbia dot edu if you would like to be on the mailing list.
Plan/References
The initial plan is to start with some foundations, from the following sources:
 BenZvi and Frenkel, Vertex algebras and algebraic curves
 di Francesco, Mathieu, Senechal, Conformal field theory
 Gawȩdzki, Lectures on conformal field theory from Quantum Fields and Strings: A Course for Mathematicians (Volume 2).
We will spend some time on (Virasoro) minimal models and Liouville theory. Then the plan is to cover aspects of WZW theory, (mainly?) following
 Etingof, Frenkel, Kirillov, Lectures on representation theory and KZ equations.
Later we may go through topics including Walgebras, the AGT correspondence, relation to geometric Langlands, and moonshine.
Schedule
Tues Sep 17  Organizational meeting 
Tues Sep 24 
Konstantin Aleshkin Introduction to CFT I will give an informal introduction to 2d CFT based on the socalled bootstrap formalism. I will introduce the main ingredients: Virasoro algebra and its representations, primary fields, BPZ equations, conformal blocks and correlation functions. My main examples will be Virasoro Minimal Models and Liouville CFT. I plan to briefly explain how other planned subjects for this seminar appear in this formalism (affine Lie algebras and KZ equations, Walgebras, AGT correspondence) if time permits. References:

Tues Oct 01 
Davis Lazowski The local structure of CFT I will introduce vertex operator algebras and relate them to the local structure of conformal field theory. 
Tues Oct 08 
Cailan Li VOA: Examples and Representations We will go over some examples of VOA and then define modules over them. We will then define vertex algebras associated to (one)dimensional lattices, in particular the free fermonic vertex superalgebra and prove the bosonfermion correspondence. 
Tues Oct 15 
Yakov Kononov Minimal models I will give an introduction to minimal models, and then answer all your questions. 
Tues Oct 22 
Guillaume Remy A probabilistic approach to Liouville conformal field theory Liouville conformal field theory is an important example of a CFT with a continuous spectrum. It was first introduced in the context of string theory by A. Polyakov in 1981 in order to understand the summation over all Riemannian metric tensors in two dimensions. In this talk I will explain how one can use probability to make rigorous the physics path integral definition of Liouville theory and define the correlation functions. We will then discuss the BPZ equations, the DOZZ formula giving the value of the threepoint function on the sphere, and if time permits, the conformal bootstrap and conformal blocks. 
Tues Oct 29 
Ivan Danilenko KZ equations 
Tues Nov 05 
Gus Schrader Free field realization, Wakimoto modules and integral solutions to KZ We will derive explicit integral formulas for the solutions of the KZ equations described by Ivan in last week's seminar. The key tool we'll use to do this is the free field realization of Wakimoto modules for affine KacMoody algebras. I'll explain some motivation behind this construction, then compute a bunch of OPE and answer all your questions. 
Thurs Nov 07 (4:306 in 507) 
Sam DeHority Representations of Quantum Affine Algebras and qKZ equations We have seen that matrix coefficients of some intertwining operators of representations of affine algebras can be interpreted as correlation functions in WZW models, and they satisfy consistent differential equations, the KZ equations. The universal enveloping algebra of an affine algebra admits a qdeformation and Frenkel and Reshetikhin have shown that matrix coefficients of intertwiners satisfy an analogous system of difference equations, which tends to the KZ equations in the limit as q goes to 1. 
Tues Nov 12 
Henry Liu An overview of AGT I'll briefly explain the physical origin of the AGT correspondence, and then do a very explicit calculation (for a free field) to equate a conformal block and a Nekrasov partition function. 
Tues Nov 19 
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Tues Nov 26 
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Tues Dec 03 
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Tues Dec 10 
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