Plan of the lectures: I. General manifold theory
Definition of a real manifold. Example : z=f(x,y) and the sphere (I
want to explain why it doesn't works with only one chart)
Definition of a tangent vector.
Why is it usually denoted by $v^i\partial_i$ ? The differential of a
map from a manifold to another. How the matrix $\frac{\partial
f^i}{\partial x^j}$ of the differential comes back in the manifold
formalism ? II. Fiber Bundle
The talk will extensively be concerned by the different ways to express
local sections of bundles.
-Definition of a vector bundle, example : the tangent bundle;
transitions functions
Sections of vector bundle; how to trivialise a section when we know a
trivialisation of the vector bundle ?
Connection of a vector bundle; local expression with respect to a
trivialisation of the bundle. Proof
:-) of the famous transformation law
$A'=g^{-1}dg+g^{-1}Ag$.
A few word about the curvature of a connection.
-Definition of a principal bundle. Example 1 : the frame bundle;
example 2 : a vector bundle is NOT a GL(V)-principal bundle.
Duality between sections and trivialisation.
Definition of a gauge transformation and a local expression.
-Definition of an associated bundle. How to trivialise an associated
bundle when we can trivialize the principal bundle ? Sections, local
expression (two forms : an equivariant function with values in the
principal bunbdle and an expression with values in the vector space).
Sketch of an answer to the most
FAQed question in the world : what is a spinor ?
Action of a gauge transformation on a section.
-Connection on principal bundle : vertical space and associated
1-form. Local expressions : the so-called "gauge potential" and its
curvature F. Why F=dA and dF=0 (famous equations !) when the group is
abelian ?
Definition of a covariant derivative on any associated bundle from a
connection on the principal bundle. The equation $D\psi=d\psi+A\psi$.
Transformation law of a connection under a gauge transformation,
transformation of a section under a gauge transformation (with a proof :-) )
Why is the covariant derivative
"covariant" ? III. Electromagnetism
Well known children formalism for the Maxwell's equations.
Why it is better to write $A=A_{\mu}dx^{\mu}$ ?
The Yang-Mills's trick as seen at the university
The Yang-Mills's trick in the bundle formalism
Spin 0 electromagnetism in a U(1)-principal bundle : gauge invariance
of the square norm of $D\phi$.
Advised references:
- S. A. Hugget and K. P. Tod "An Introduction to Twistor
Geometry", Cambridge University Press
- R. S. Ward and R. O. Wells "Twistor Geometry and Field
Theory", Cambridge University Press
Main references (see the lecture notes for a full list
of references):
-P. Candelas, "Lectures on complex geometry", in Trieste 1987,
Proceedings, Superstrings '87. 1987.
-K. Hori et al, Mirror Symmetry, vol.1 of Clay Mathematics Monographs.
American Mathematical Society, 2003. 929 p.
-T. Hubsch, Calabi-Yau manifolds: a bestiary for physicists. World
Scientific, 1992. 374 p.
-D. D. Joyce, Compact manifolds with
special holonomy. Oxford Mathematical Monographs. Oxford
University Press, 2000. 436 p.
-M. Nakahara, Geometry, topology and
physics. The Institute of Physics, 2002. 520 p.
-H. Skarke, "String dualities and toric geometry: an introduction,"
arXiv:hep-th/9806059.
Plan of the lectures: part I: Structure of semi-simple complex Lie algebras
- basic definitions
- The Cartan-Weyl basis
- The Killing form
- Simple roots, Cartan matrix, Dynkin diagrams
- The Chevalley basis
- Weyl group part II: Representation theory
- Fondamental and highest weights
- Freudenthal recursion formula
- Racah-Speiser algorithm
- Weyl's character formula and dimensionality formula part III: Applications to A_2, the complexification of su(3) part IV: Clifford algebra
-Gamma matrices: in even dimension, in odd dimension, Lorentz
transformations, crucial identities for SYM
-Spinors: Weyl spinor, Majorana spinor, Majorana-Weyl spinor
-Majorana representation and SO(8) triolity
part V:Universal enveloping algebras and higher symmetries
- Some taste of abstract Algebra
* Free, tensor, symmetric
* Associative vs Lie : Universal enveloping
- Physical applications
* Casimir operators
* Higher symmetries
Advised references:
-J.E.Humphreys, "Introduction to Lie algebras and representation
theory", Graduate texts in Mathematics 9, Springer Verlag (2000).
-J.F.Cornwell, "Group theory in physics: An introduction", San
Diego, USA: Academics (1997).
-J. Fuchs and C. Schweigert, "Symmetries, Lie Algebras and
Representations:A graduate course for physicists", Cambridge, UK,
University Press (1997).
-W.Fulton and J.Harris, "Representation Theory: A First Course",
Springer Verlag (1991) 3rd Edition.
-Kugo and Townsend, Nucl. Phys. B221: 357, 1983
Plan of the lectures: Conformal field theory in two dimensions
- local/global conformal transformations, primary/quasi-primary fields
- conformal Ward identities, operator product expansion
- Energy momentum tensor as generator of conformal symmetry
- radial and conformal normal orderings
- Field/state correspondance
- Virasoro algebra, Verma modules
Advised references:
- Conformal field theory (P Di Francesco, P Mathieu, D Senechal,New
York, USA: Springer (1997) ), Chap. 4,5,6,15 essentially
- Introduction to conformal field theory, AN Schellekens ,Fortsch.
Phys, 1996, http://staff.science.uva.nl/~jdeboer/stringtheory/CFT.ps
- Some reviews on the arXiv, see e.g. Ginsparg (hep-th/9108028),
Gaberdiel (hep-th/9910156), Walton (hep-th/9911187) and more...
Background material:
Some basic knowledge of Quantum Field Theory (Poincare invariance,
Noether's theorem, correlation functions, ...). Chapter 2 of the first
reference provides a good idea of what we will need!
Plan of the lectures: I. Brief review of field quantization and perturbation
theory II. One loop calculations in phi4
theory and QED including renormalization. III. Renormalization
and Symmetry: The axial anomaly. IV. Renormalization group: i) Callan-Symanzik beta and
gamma functions
ii) Evolution of couplings
iii) Wilson approach.