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We consider a lattice model of a semiflexible homopolymer chain in a badsolvent. Beside the temperature $T$, this model is described by (i) a curvatureenergy $\varepsilon_h$, representing the stiffness of the chain (ii) anearest-neighbour attractive energy $\varepsilon_v$, representing the solvent(iii) the monomer density $\rho={N \over \Omega}$, where $N$ and $\Omega$denote respectively the number of monomers and the number of lattice sites.This model is a simplified view of the protein folding problem, whichencompasses the geometrical competition between secondary structures (thecurvature term modelling helix formation) and the global compactness (modeledhere by the attractive energy), but contains no side chain information...Comment: 17 pages, plain tex, 2 figures available upon reques

Phase diagram of a semiflexible polymer chain in a θ solvent: Application to protein folding