For the simple theory of a single real scalar field $\phi$ in 1+1D, the Lagrange density is $$\mathcal{L}=\frac{1}{2}\partial_\mu\phi\partial^\mu\phi-U(\phi)\tag{1}$$ with Minkowski signature $(+,-)$, and the corresponding Hamiltonian is $$\mathcal{H}=\frac{1}{2}\partial_\mu\phi\partial^\mu\phi+U...