  Different AdS-Rindler wedges can be mapped to each other using bulk
isometries. In this paper we address how the boundary representations
corresponding to the AdS-Rindler wedges transform under such isometries. We
show that when a bulk wedge is mapped to another using a bulk isometry, their
boundary representations are mapped by the conformal transformation
corresponding to the isometry. We comment on the import of this result on the
relation between AdS/CFT and quantum error correction.
