We consider a quenched-disordered heteropolymer, consisting of
hydrophobic and hydrophylic monomers, in the vicinity of an oil-water
interface. The heteropolymer is modeled by a directed simple random walk$(i,
S_i)_{i\epsilon\mathbb{N}}$ on $\mathbb{N} \times \mathbb{Z}$ with an
interaction given by the Hamiltonians $H_n^{\omega}(S) = \lambda
\Sigma_{i=1}^n(\omega_i + h)\text{sign}(S_i)(n \epsilon \mathbb{N})$. Here,
$\lambda$ and h are parameters and $(\omega_i)_{i\epsilon\mathbb{N}}$
are i.i.d. $\pm1$-valued random variables. The sign $(S_i) = \pm1$ indicates
whether the ith monomer is above or below the interface, the $\omega_i =
\pm1$ indicates whether the ith monomer is hydrophobic or hydrophylic.
It was shown by Bolthausen and den Hollander that the free energy exhibits a
localization-delocalization phase transition at a curve in the $(\lambda,
h)$-plane.
¶ In the present paper we show that the free-energy localization
concept is equivalent to pathwise localization. In particular, we prove that
free-energy localization implies exponential tightness of the polymer
excursions away from the interface, strictly positive density of intersections
with the interface and convergence of ergodic averages along the polymer. We
include an argument due to G. Giacomin, showing that free-energy delocalization
implies that there is pathwise delocalization in a certain weak sense.