In Evans's PDE (on page 588), in the proof of a uniqueness result for viscosity solutions of the Hamilton-Jacobi equation, it is claimed that there exists the maximum
$$\max_{\mathbb{R}^{2n}\times (0,\infty)^2} \Phi(x,y,t,s) = \max_{\mathbb{R}^{2n}\times (0,\infty)^2} u(x,t) - v(y,s) - \lambda (t+s) - \frac{1}{\epsilon^2}(|x-y|^2+(t-s)^2) -\epsilon(|x|^2+|y|^2)$$ where $\epsilon>0$, $\lambda < 1$ and $u$ and $v$ are bounded and uniformly continuous (and viscosity solutions of an Hamilton-Jacobi equation).
Can you explain to me in detail the following points?
- Why does that maximum exist?
- What's the motivation of the penalization terms?
Let $M$ be a bound for $|u|$ and $|v|$. For $R>0$, if $t, s \geq R$ and $|x|^2+|y|^2 \geq R$, you have that $\Phi(t,s,x,y) \leq 2M - (\lambda + \epsilon)R$, and the r.h.s. goes to $-\infty$ as $R\to +\infty$. Hence there exists $R>0$ such that $$ \Phi(t,s,x,y) \leq \Phi(0,0,0,0)\qquad \forall t,s\geq R,\ \forall (x,y):\ |x|^2 + |y|^2\geq R. $$ In particular, the continuous function $\Phi$ reaches its maximum on the compact set $\{(t,s,x,y):\ t,s\in [0, R],\ |x|^2+|y|^2 \leq R\}$.
This explains the presence of the penalization terms $-\lambda(t+s)$ and $-\epsilon(|x|^2 + |y|^2)$.
The other penalization term $$ -\frac{1}{\epsilon^2} (|x-y|^2 + |t-s|^2) $$ is a standard term in all the proofs based on the Kruzkov's doubling of variables technique. Heuristically, you see that as $\epsilon\to 0$ you need to have $|x_\epsilon - y_\epsilon|$ and $|t_\epsilon - s_\epsilon|$ very small at maximum points $(t_\epsilon, s_\epsilon, x_\epsilon, y_\epsilon)$ of $\Phi$. If you go through Evans' proof, this fact is seen for instance in formula (11).