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Lectures on String Theory

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– 140 –<br />

as<br />

Here<br />

Exercise 50. Under finite transformati<strong>on</strong>s z → f(z) the stress tensor transforms<br />

T (z) → T ′ (z) = (∂f) 2 T (f(z)) + c<br />

12 D(f) z<br />

D(f) z = ∂f(z)∂3 f(z) − 3 2 (∂2 f(z)) 2<br />

(∂f) 2<br />

is the Schwarzian derivative. Show that if f(z) = az+b<br />

cz+d then D(f) z = 0.<br />

Exercise 51. C<strong>on</strong>sider a parallelogram <strong>on</strong> the complex plane determined by the<br />

following identificati<strong>on</strong><br />

z ≡ z + nλ 1 + mλ 2 ,<br />

n, m ∈ Z<br />

Show that a general transformati<strong>on</strong><br />

λ 1 → dλ 1 + cλ 2 , λ 2 → bλ 1 + aλ 2<br />

with the c<strong>on</strong>diti<strong>on</strong> ad − bc = 1 preserves the area of the parallelogram.<br />

Exercise 52. Show that the modular transformati<strong>on</strong>s<br />

T : τ → τ + 1 , S : τ → − 1 τ<br />

applied to the fundamental regi<strong>on</strong> of the modular group<br />

{<br />

M g=1 = − 1 2 ≤ Reτ ≤ 0, |τ|2 ≥ 1 ∪ 0 < Reτ < 1 }<br />

2 , |τ|2 > 1<br />

generate the whole upper-half plane.<br />

Exercise 53. Show that τ = i and τ = e 2πi<br />

3 are the fixed points of S and ST<br />

transformati<strong>on</strong>s respectively.<br />

Exercise 54. Verify that the acti<strong>on</strong><br />

S = − 1 ∫<br />

d 2 σ<br />

(∂ α X µ ∂ α X µ + 2i<br />

8π<br />

¯ψ<br />

)<br />

µ ρ α ∂ α ψ µ .<br />

is invariant under supersymmetry transformati<strong>on</strong>s w<br />

δ ɛ X µ = i¯ɛψ µ ,<br />

δ ɛ ψ µ = 1 2 ρα ∂ α X µ ɛ<br />

δ ɛ ¯ψµ = − 1 2¯ɛρα ∂ α X µ

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