The delocalization and unbinding transitions of two semi-flexible polymers
which experience attractive interactions are studied by a variety of theore
tical methods. In two-dimensional systems, one has to distinguish four diff
erent universality classes for the interaction potentials. In particular, t
he delocalization transitions from a potential well and the unbinding trans
itions from such a well in the presence of a hard wall exhibit distinct cri
tical behavior governed by different critical exponents. In three-dimension
al systems! we predict first-order transitions with a jump in the energy de
nsity but with critical or self-similar fluctuations leading to distributio
n functions with poser law tails. The predicted critical behavior is confir
med numerically by transfer matrix calculations in two dimensions and by Mo
nte Carlo simulations in three dimensions. This behavior should be accessib
le to experiments on biopolymers such as actin filaments or microtubuli.