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Lectures on String Theory

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Exercise 45. C<strong>on</strong>sider c<strong>on</strong>formal transformati<strong>on</strong>s z → z ′ = f(z). By definiti<strong>on</strong>,<br />

primary fields are the fields which transform as tensors under c<strong>on</strong>formal transformati<strong>on</strong>s<br />

( ∂z<br />

φ(z, ¯z) → φ ′ ′ ) h ( ∂¯z<br />

′ )¯hφ(z<br />

(z, ¯z) =<br />

′ (z), ¯z ′ (¯z))<br />

∂z ∂¯z<br />

Find how a primary field transforms under infinitezimal c<strong>on</strong>formal transformati<strong>on</strong>s<br />

φ → φ + δ ξ,¯ξφ, where z ′ = z + ξ(z).<br />

Exercise 46. Show that c<strong>on</strong>formal fields of weight h have the following mode<br />

expansi<strong>on</strong><br />

φ(z) =<br />

∑<br />

z −n−h φ n .<br />

n∈integer<br />

Exercise 47. In the radial quantizati<strong>on</strong> products of fields is defined by putting<br />

them in the radial order. Using the radial order prescripti<strong>on</strong> show that the c<strong>on</strong>formal<br />

transformati<strong>on</strong><br />

δ ξ φ(w) = [T ξ , φ(w)]<br />

can be written in the form<br />

∮<br />

δ ξ φ(w) =<br />

C w<br />

dz<br />

ξ(z)T (z)φ(w)<br />

2πi<br />

Here C w is a small c<strong>on</strong>tour in a complex plane around point z.<br />

Exercise 48.<br />

formula<br />

Using the previous exercise together with the Cauchy-Riemann<br />

∮<br />

C w<br />

dz f(z)<br />

2πi (z − w) = f (n−1) (w)<br />

n (n − 1)!<br />

show that any c<strong>on</strong>formal field must have the following R-ordered operator product<br />

with T (z):<br />

T (z)φ(w) =<br />

hφ(w)<br />

(z − w) + ∂φ(w) + regular terms<br />

2 (z − w)<br />

Exercise 49. Show that the following operator product of the stress tensor<br />

T (z)T (w) = c/2 2T (w) ∂T (w)<br />

+ +<br />

(z − w)<br />

4<br />

(z − w)<br />

2<br />

(z − w)<br />

+ regular terms<br />

corresp<strong>on</strong>ds to the following transformati<strong>on</strong> law<br />

δ ξ T (z) = c<br />

12 ∂3 ξ(z) + 2∂ξ(z)T (z) + ξ(z)∂T (z)

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