Proof.
We first prove the equivalence between 1 and 1 when $\varphi ,\psi \in \mathrm{PSH}(X,\theta )_{>0}$.
1 $\implies $ 1. Assume that $\varphi \sim _ P \psi $. By 16.8.4, we have
\[ P_{\theta }[\varphi ]=P_{\theta }[\psi ]. \]
So 1 follows from proposition 16.3.10.
1 $\implies $ 1. Since $\varphi \preceq _ P\psi $, we have $P_{\theta }[\varphi ]\leq P_{\theta }[\psi ]$. Moreover, proposition 16.3.10 shows that $P_{\theta }[\varphi ]$ and $P_{\theta }[\psi ]$ have the same positive mass. By theorem 16.3.15, $P_{\theta }[\psi ]$ is a candidate in the characterization of $P_{\theta }\bigl [P_{\theta }[\varphi ]\bigr ]=P_{\theta }[\varphi ]$. Hence $P_{\theta }[\psi ]\leq P_{\theta }[\varphi ]$, and therefore $P_{\theta }[\varphi ]=P_{\theta }[\psi ]$. So 1 follows.
Let us come back to the general case with $\varphi ,\psi \in \mathrm{PSH}(X,\theta )$.
1 $\implies $ 2. Fix $j\in \{ 0,\ldots ,n\} $. We argue (16.8.8).
Take a Kähler form $\omega $ on $X$. By 16.8.4, for each $\epsilon >0$, we have
\[ P_{\theta +\epsilon \omega }[\varphi ]= P_{\theta +\epsilon \omega }[\psi ]. \]
It follows from proposition 16.3.10 that
\[ \begin{aligned} \int _ X \left(\theta +\epsilon \omega +\mathrm{dd}^{\mathrm{c}}\psi \right)^ j\wedge \theta _{V_{\theta }}^{n-j}=& \int _ X \Bigl (\theta +\epsilon \omega +\mathrm{dd}^{\mathrm{c}}P_{\theta +\epsilon \omega }[\psi ] \Bigr )^ j\wedge \theta _{V_{\theta }}^{n-j}\\ =& \int _ X \Bigl (\theta +\epsilon \omega +\mathrm{dd}^{\mathrm{c}}P_{\theta +\epsilon \omega }[\varphi ] \Bigr )^ j\wedge \theta _{V_{\theta }}^{n-j} \\ =& \int _ X \left(\theta +\epsilon \omega +\mathrm{dd}^{\mathrm{c}}\varphi \right)^ j\wedge \theta _{V_{\theta }}^{n-j}. \end{aligned} \]
Since the two extremes are both polynomials in $\epsilon $ by the multi-linearity of the non-pluripolar products proposition 13.11.4 6, we conclude that the same holds when $\epsilon =0$, that is, (16.8.8) holds.
2 $\implies $ 1. Assume (16.8.8) holds for all $j=0,\ldots ,n$. Then the same holds with $P_{\theta }[\psi ]$ in place of $\psi $, thanks to proposition 16.3.10. Therefore, for each $t\in (0,1)$, we have
\[ \int _ X \theta _{t\varphi +(1-t)V_{\theta }}^ n= \int _ X \theta _{tP_{\theta }[\psi ]+(1-t)V_{\theta }}^ n \]
by the binomial expansion. Furthermore, $t\varphi +(1-t)V_{\theta }\preceq tP_{\theta }[\psi ]+(1-t)V_{\theta }$. By the implication 1 $\implies $ 1, we have
\[ t\varphi +(1-t)V_{\theta }\sim _ P t P_{\theta }[\psi ]+(1-t)V_{\theta } \]
for each $t\in (0,1)$.
Fix a Kähler form $\omega $ on $X$. From the implication 1 $\implies $ 1, we have
\[ \int _ X (\theta +\omega )_{t\varphi +(1-t)V_{\theta }}^ n= \int _ X (\theta +\omega )_{tP_{\theta }[\psi ]+(1-t)V_{\theta }}^ n. \]
Since both sides are polynomials in $t$ by the multi-linearity of the non-pluripolar products proposition 13.11.4 6, the same holds when $t=1$. From the implication 1 $\implies $ 1 again, we have $\varphi \sim _ P P_{\theta }[\psi ]\sim _ P \psi $.
$\square$
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