Cargando…

TASI lectures on AdS/CFT

We introduce the AdS/CFT correspondence as a natural extension of QFT in a fixed AdS background. We start by reviewing some general concepts of CFT, including the embedding space formalism. We then consider QFT in a fixed AdS background and show that one can define boundary operators that enjoy very...

Descripción completa

Detalles Bibliográficos
Autor principal: Penedones, Joao
Lenguaje:eng
Publicado: 2016
Materias:
Acceso en línea:https://dx.doi.org/10.1142/9789813149441_0002
http://cds.cern.ch/record/2208920
_version_ 1780951746578743296
author Penedones, Joao
author_facet Penedones, Joao
author_sort Penedones, Joao
collection CERN
description We introduce the AdS/CFT correspondence as a natural extension of QFT in a fixed AdS background. We start by reviewing some general concepts of CFT, including the embedding space formalism. We then consider QFT in a fixed AdS background and show that one can define boundary operators that enjoy very similar properties as in a CFT, except for the lack of a stress tensor. Including a dynamical metric in AdS generates a boundary stress tensor and completes the CFT axioms. We also discuss some applications of the bulk geometric intuition to strongly coupled QFT. Finally, we end with a review of the main properties of Mellin amplitudes for CFT correlation functions and their uses in the context of AdS/CFT.
id cern-2208920
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2016
record_format invenio
spelling cern-22089202021-05-03T20:23:24Zdoi:10.1142/9789813149441_0002http://cds.cern.ch/record/2208920engPenedones, JoaoTASI lectures on AdS/CFTParticle Physics - TheoryWe introduce the AdS/CFT correspondence as a natural extension of QFT in a fixed AdS background. We start by reviewing some general concepts of CFT, including the embedding space formalism. We then consider QFT in a fixed AdS background and show that one can define boundary operators that enjoy very similar properties as in a CFT, except for the lack of a stress tensor. Including a dynamical metric in AdS generates a boundary stress tensor and completes the CFT axioms. We also discuss some applications of the bulk geometric intuition to strongly coupled QFT. Finally, we end with a review of the main properties of Mellin amplitudes for CFT correlation functions and their uses in the context of AdS/CFT.We introduce the AdS/CFT correspondence as a natural extension of QFT in a fixed AdS background. We start by reviewing some general concepts of CFT, including the embedding space formalism. We then consider QFT in a fixed AdS background and show that one can define boundary operators that enjoy very similar properties as in a CFT, except for the lack of a stress tensor. Including a dynamical metric in AdS generates a boundary stress tensor and completes the CFT axioms. We also discuss some applications of the bulk geometric intuition to strongly coupled QFT. Finally, we end with a review of the main properties of Mellin amplitudes for CFT correlation functions and their uses in the context of AdS/CFT.arXiv:1608.04948oai:cds.cern.ch:22089202016-08-17
spellingShingle Particle Physics - Theory
Penedones, Joao
TASI lectures on AdS/CFT
title TASI lectures on AdS/CFT
title_full TASI lectures on AdS/CFT
title_fullStr TASI lectures on AdS/CFT
title_full_unstemmed TASI lectures on AdS/CFT
title_short TASI lectures on AdS/CFT
title_sort tasi lectures on ads/cft
topic Particle Physics - Theory
url https://dx.doi.org/10.1142/9789813149441_0002
http://cds.cern.ch/record/2208920
work_keys_str_mv AT penedonesjoao tasilecturesonadscft