We consider a potential W:RmβR with two different global minima
aββ,a+β and, under a symmetry assumption, we use a variational approach to
show that the Hamiltonian system \begin{equation} \ddot{u}=W_u(u), \hskip 2cm
(1) \end{equation} has a family of T-periodic solutions uT which, along a
sequence Tjββ+β, converges locally to a heteroclinic solution
that connects aββ to a+β. We then focus on the elliptic system
\begin{equation} \Delta u=W_u(u),\;\; u:R^2\rightarrow R^m, \hskip 2cm (2)
\end{equation} that we interpret as an infinite dimensional analogous of (1),
where x plays the role of time and W is replaced by the action functional
JRβ(u)=β«Rβ(21ββ£uyββ£2+W(u))dy. We assume that
JRβ has two different global minimizers uΛββ,uΛ+β:RβRm in the set of maps that connect aββ to a+β. We work in a symmetric
context and prove, via a minimization procedure, that (2) has a family of
solutions uL:R2βRm, which is L-periodic in x, converges to
aΒ±β as yβΒ±β and, along a sequence
Ljββ+β, converges locally to a heteroclinic solution that
connects uΛββ to uΛ+β.Comment: 36 pages, 4 figure