We consider a potential W:Rm→R with two different global minima
a−,a+ 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 Tj→+∞, converges locally to a heteroclinic solution
that connects a− to a+. 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
JR(u)=∫R(21∣uy∣2+W(u))dy. We assume that
JR has two different global minimizers uˉ−,uˉ+:R→Rm in the set of maps that connect a− to a+. We work in a symmetric
context and prove, via a minimization procedure, that (2) has a family of
solutions uL:R2→Rm, which is L-periodic in x, converges to
a± as y→±∞ and, along a sequence
Lj→+∞, converges locally to a heteroclinic solution that
connects uˉ− to uˉ+.Comment: 36 pages, 4 figure