Polyakov Action - Global Symmetries

Global Symmetries

N.B. : Here, a symmetry is said to be local or global from the two dimensional theory (on the worldsheet) point of view. For example, Lorentz transformations, that are local symmetries of the space-time, are global symmetries of the theory on the worldsheet.

The action is invariant under spacetime translations and infinitesimal Lorentz transformations:

(i)
(ii)

where and is a constant. This forms the Poincaré symmetry of the target manifold.

The invariance under (i) follows since the action depends only on the first derivative of . The proof of the invariance under (ii) is as follows:

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