Since the gauge group underlying (2 + 1)-dimensional general relativit
y is noncompact, certain difficulties arise in the passage from the co
nnection to the loop representations. It is shown that these problems
can be handled by appropriately choosing the measure that features in
the definition of the loop transform. Thus, 'old-fashioned' loop repre
sentations-based on ordinary loops-do exist. In the case when the spat
ial topology is that of a 2-torus, these can be constructed explicitly
; all quantum states can be represented as functions of (homotopy clas
ses of) loops and the scalar product and the action of the basic obser
vables can be given directly in terms of loops.