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Lectures on Supergravity Joaquim Gomis Based on the SUGRA book of Dan Freedman and Antoine Van Proeyen to appear in Cambridge University Press

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Page 1: I-Supergravity1-29.pdf

Lectures on Supergravity

Joaquim GomisBased on the SUGRA book of Dan Freedman

and Antoine Van Proeyen to appear in Cambridge University Press

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Public Material

Lectures on supergravity, Amsterdam-Brussels-Paris doctoral school, Paris 2009, October-November 2009: PDF-file.

http://itf.fys.kuleuven.be/~toine/SUGRA_DoctSchool.pdf

A. Van Proeyen, Tools for supersymmetry, hep-th 9910030

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History and overview ofSupergravity

60’ and 70’s. Yang Mills theories, Spontaneous symmetry breaking. Standard model

Supersymmetry

Yu. Gol’fand , E. Lichtman (1971)J.L. Gervais and B. Sakita (1971)A,Neveu, J. Schwarz, P.Ramond (1971)D. Volkov, V. Akulov (1972)J. Wess, B. Zumino (1974)

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History and overview ofSupergravity

• Yu. Gol’fand , E. Lichtman- Parity violation in QFT, 4d• J.L. Gervais and B. Sakita & A,Neveu, J. Schwarz String theory-Dual

models. Worls sheet supersymmetry 2d• D. Volkov, V. Akulov- Goldstone particles of spin ½? 4d• J. Wess, B. Zumino Supersymmetric field theory in 4d

Supergroup, superalgebra

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History and overview ofSupergravity

• Super Poincare

Translations

Spinor supercharge

Lorentz transformations

Massless multiplets contains spins (s, s-1/2), for s=1/2, 1, 2,

R symmetry

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History and overview ofSupergravity

Supergravity

Gauged supersymmetry was expected to be an extension of generalRelativity with a superpartner of the gravito call gravition

Multiplet (2,3/2)

S. Ferrara, D. Freedman, P. Van Nieuwenhuizen (1976)S. Deser, B. Zumino (1976)D. Volkov, V. Soroka (1973), massive gravitinos,..

Extensions with more supersymmetries and extension has beenconsidered, N=2 supergravity, special geometry. N=1 Supergravity in 11d

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Motivation for Supergravity

Supergravity (SUGRA) is an extension of Einstein's general relativity to include supersymmetry (SUSY). General relativity demands extensions since it has shortcomings including at least the following:

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Motivation for Supergravity• Space time singularities. The singularity theorems of Penrose,

Hawking and Geroch shows that general relativity is incomplete.

• Failure to unify gravity with the strong and electro weak forces.

• Einstein gravity is not power counting renormalizable. It is renormalizable as an effective theory. It is not a fundamental theory

• If we include supersymmetry in a theory of gravity. The simple example of divergences: zero point energy of the vacuum, can potentially be cancelled by super partners of ordinary particles

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The current status of supergravity

• A reliable approximation to M-theory.• An essential ingrediente for supersymmetric

phenomenology ( minimal supersymmetricestándar model coupled to N=1 supergravity).

• Applications in cosmology• An crucial part for the AdS/CFT correspondence

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Index

• Scalar field and its symmetries• The Dirac Field• Clifford algebras ans spinors• The Maxwell and Yang-Mills Gauge fields• Free Rarita-Schwinger field• Differential geometry• First and second order formulation of gravity• N=1 Global Supersymmetry in D=4

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Index

• N=1 pure supergravity in 4 dimensions• D=11 supergravity

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Scalar field

Noether symmetry leaves the action invariant

Symmetry transformations

Metric (-,+,+,+…+)

map solutions into solutions

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General internal symmetry

Infinitesimal transformations

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General internal symmetryCommutator of infinitesimal transformations

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Spacetime symmetries

Vector representation

Relations among Lorentz transformations

Lorentz condition

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Spacetime symmetries

Orbital part

Lorentz algebra

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Noether chargesInfinitesimal Noether symmetry

Noether current

Noether trick. Consider

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Noether charges

Hamiltonian formalism

For internal symmetries

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Noether charges

At quantum level

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The fundamental spinor representations

The transformation induces a Lorentz transformation

Properties

Hermitean matrix

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The Dirac Field

Applying the Dirac operator

Clifford algebra

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The Dirac FieldExplicit representation for D=4 in terms of

Finite Lorentz transformations

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The Dirac Field

Dirac action

Equation of motion for adjoint spinor

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Weyl spinors

Undotted components

Dotted components

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Weyl spinors

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Energy momentum tensor

where

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Clifford algebras and spinors

• Clifford algebras in general dimensions

Euclidean Clifford algebras

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Clifford algebras and spinors