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Lectures on String Theory

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– 141 –<br />

provided the parameter ɛ satisfies the following equati<strong>on</strong><br />

ρ β ρ α ∂ β ɛ = 0 .<br />

Exercise 55. If in the previous exercise the parameter ɛ is c<strong>on</strong>stant then we<br />

deal with global supersymmetry transformati<strong>on</strong>s. Derive the Noether current which<br />

corresp<strong>on</strong>ds to this global symmetry of the acti<strong>on</strong>.<br />

Exercise 56*. Express the spin c<strong>on</strong>necti<strong>on</strong> ω via vielbein e by using the c<strong>on</strong>diti<strong>on</strong><br />

of vanishing of the torsi<strong>on</strong><br />

T a αβ = D α e a β − D β e a α = 0 .<br />

Exercise 57. Derive the <strong>on</strong>-shell algebra of supersymmetry transformati<strong>on</strong>s<br />

[δ 1 , δ 2 ] =? .<br />

Exercise 58. Using the Noether method derive the currents corresp<strong>on</strong>ding to<br />

the Poincaré symmetry for the fermi<strong>on</strong>ic string. Express the corresp<strong>on</strong>ding Noether<br />

charges via oscillators for both Neveuw-Schwarz and Ram<strong>on</strong>d sectors.

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