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Minimal lectures on two-dimensional conformal field theory

by Sylvain Ribault

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Submission summary

Authors (as registered SciPost users): Sylvain Ribault
Submission information
Preprint Link: http://arxiv.org/abs/1609.09523v4  (pdf)
Date accepted: Jan. 18, 2018
Date submitted: Jan. 15, 2018, 1 a.m.
Submitted by: Sylvain Ribault
Submitted to: SciPost Physics Lecture Notes
Ontological classification
Academic field: Physics
Specialties:
  • High-Energy Physics - Theory
  • Mathematical Physics
Approach: Theoretical

Abstract

We provide a brief but self-contained review of conformal field theory on the Riemann sphere. We first introduce general axioms such as local conformal invariance, and derive Ward identities and BPZ equations. We then define minimal models and Liouville theory by specific axioms on their spectrums and degenerate fields. We solve these theories by computing three- and four-point functions, and discuss their existence and uniqueness.

Author comments upon resubmission

I have made a number of relatively minor changes.

List of changes

Reply to Reviewer 1: The typo after (3.15) is now corrected.

Reply to Reviewer 3:

  1. There was indeed a contradition because Axiom 3.4 was too strong. I have modified that Axiom so that it applies only to fields that correspond to states in the spectrum. Then OPEs of degenerate fields are not covered, and should be discussed separately. I have added such a discussion after Axiom 4.10.

  2. I have added a paragraph at the very end of Section 5, in order to make contact with the original definition (and naming) of Liouville theory, and to refer the reader to ref. [3] for more details.

  3. I have added a paragraph between eqs. (4.10) and (4.11) in order to further discuss the guess for the lower bound, and to mention the alternative guess that the lower bound could be zero.

  4. Between eqs. (5.18) and (5.19), I have amended the discussion of invariance under field renormalization: it is now stated that invariant quantities are sufficient for checking crossing symmetry, and explained why we may want to choose a normalization.

Additional changes:

  1. At the end of the introduction, I have added a further motivation for the minimalistic approach, namely that it can be useful in research on other CFTs. Reference [6] is given as an example.

  2. In Exercise 3.5, I have added substantial hints.

Published as SciPost Phys. Lect. Notes 1 (2018)

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