We study the following quasilinear elliptic system for all
\begin{equation*} \label{}
-div(\Phi’(|\nabla u_i|^2) \nabla u_i) = H_i(u) \quad \
^n
\end{equation*} where and the
nonlinearity is a general
nonlinearity. Several celebrated operators such as the prescribed mean
curvature, the Laplacian and the -Laplacian operators fit in the above form,
for appropriate . We establish a Hamiltonian identity of the following
form for all \begin{equation*}\label{} \int_{\mathbb R^{n-1}}
\left(\sum_{i=1}^{m} \left[ \frac{1}{2} \Phi\left(|\nabla u_i|^2\right) -
\Phi’\left(|\nabla u_i|^2\right) |\partial_{x_n} u_i|^2 \right] - \tilde H(u)
\right) d x’\equiv C, \end{equation*} where and
is the antiderivative of . This can be seen as a
counterpart of celebrated pointwise inequalities provided by Caffarelli,
Garofalo and Segala in \cite{cgs} and by Modica in \cite{m}. For the case of
system of equations, that is when , we show that as long as the
function $I_\alpha®:=\frac{1}{r^{n-\alpha}} \int_{B_r} \sum_{i=1}^{m}
\Phi(|\nabla u_i|^2) - 2\tilde H(u)r$. We call
this a weak monotonicity formula since for it is shown in \cite{cgs} that
is monotone when , under certain conditions on
. We prove De Giorgi type results and Liouville theorems for -monotone
and stable solutions in two and three dimensions when the system is symmetric.

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