I'm reading the proof of Kantorovich duality from Villani's book Topics in Optimal Transportation. In page 28, the author said that
Exercise 1.11. Let us try to extend this proof to the non-compact case. Why would we like to replace $C_{b}(X \times Y)$ by $C_{0}(X \times Y) ?$ Show that if we do so in the definition of $\Xi$, then the latter turns out to be trivial: $\Xi \equiv 0$. This shows that the proof as such does not work in a non-compact setting. Still, a variation of it can be used, as we shall see later in Appendix 1.3.
Let $X$ and $Y$ be Polish spaces. Let $E:=C_{0}(X \times Y)$ be the space of all continuous vanishing at infinity functions on $X \times Y$, equipped with its usual supremum norm $\|\cdot\|_{\infty}$. Let $$ \Xi: u \in E \longmapsto\left\{\begin{array}{l} \int_{X} \varphi d \mu+\int_{Y} \psi d \nu &\begin{align*} &\text {if } u = \varphi \oplus \psi \text{ for some } (\varphi, \psi) \in C_b(X) \times C_b(Y) \end{align*}\\ +\infty &\text {else. } \end{array}\right. $$
I could not see how $\Xi \equiv 0$. For example, take some $(\varphi, \psi) \in C_0(X) \times C_0(Y)$. Then define $u$ by $u (x,y) := \varphi(x)+ \psi(y)$. Then $u \in E$. However, $\int_{X} \varphi d \mu+\int_{Y} \psi d \nu$ is possibly nonzero.
Could you explain why $\Xi \equiv 0$ if $E=C_{0}(X \times Y)$?