Abstract
The string equivalent of a massless particle () is the tensionless string (). The study of such strings is of interest when trying to understand the high energy limit of ordinary strings. I discuss the classical limit of the bosonic string, the spinning string and the superstring. A common feature is the appearence of a space-time (super-)conformal symmetry replacing the world-sheet Weyl invariance. The question of whether this symmetry may survive quantization is addressed. A lightcone analysis of the quantized bosonic tensionless string leads to severe constraints on the physical states: they are space-time diffeomorphism singlets characterized by their topological properties only.
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