Lectures on String Theory
Lectures on String Theory
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)