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Chapter 2<br />

Basics in <strong>Conformal</strong> <strong>Field</strong> <strong>Theory</strong><br />

The approach for studying conformal field theories is somewhat different from the<br />

usual approach for quantum field theories. Because, instead of starting with a classical<br />

action for the fields and quantising them via the canonical quantisation or the<br />

path integral method, one employs the symmetries of the theory. In the spirit of<br />

the so-called boot-strap approach, for CFTs one defines and for certain cases even<br />

solves the theory just by exploiting the consequences of the symmetries. Such a procedure<br />

is possible in two dimensions because the algebra of infinitesimal conformal<br />

transformations in this case is very special: it is infinite dimensional.<br />

In this chapter, we will introduce the basic notions of two-dimensional conformal<br />

field theory from a rather abstract point of view. However, in Sect. 2.9, we will study<br />

in detail three simple examples important for string theory which are given by a<br />

Lagrangian action.<br />

2.1 The <strong>Conformal</strong> Group<br />

We start by introducing conformal transformations and determining the condition<br />

for conformal invariance. Next, we are going <strong>to</strong> consider flat space in d ≥ 3dimensions<br />

and identify the conformal group. Finally, we study in detail the case<br />

of Euclidean two-dimensional flat space R 2,0 and determine the conformal group<br />

and the algebra of infinitesimal conformal transformations. We also comment on<br />

two-dimensional Minkowski space R 1,1 in the end.<br />

2.1.1 <strong>Conformal</strong> Invariance<br />

<strong>Conformal</strong> Transformations<br />

Let us consider a flat space in d dimensions and transformations thereof which locally<br />

preserve the angle between any two lines. Such transformations are illustrated<br />

in Fig. 2.1 and are called conformal transformations.<br />

In more mathematical terms, a conformal transformation is defined as follows.<br />

Let us consider differentiable maps ϕ : U → V , where U ⊂ M and V ⊂ M ′ are<br />

Blumenhagen, R., Plauschinn, E.: Basics in <strong>Conformal</strong> <strong>Field</strong> <strong>Theory</strong>. Lect. Notes Phys. 779, 5–86<br />

(2009)<br />

DOI 10.1007/978-3-642-00450-6 2 c○ Springer-Verlag Berlin Heidelberg 2009

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