Let
- $(E,\mathcal E,\lambda)$ be a measure space
- $p:E\to[0,\infty)$ be $\mathcal E$-measurable with $$c:=\int p\:{\rm d}\lambda\in(0,\infty)$$ and $$\mu:=\underbrace{\frac1cp}_{=:\:\tilde p}\lambda$$
- $q:E^2\to[0,\infty)$ be ${\mathcal E}^{\otimes2}$-measurable and $$Q(x,\;\cdot\;)=q(x,\;\cdot\;)\lambda\;\;\;\text{for }x\in E$$
- $(\Omega,\mathcal A,\operatorname P)$ be a probability space
- $X$ be an $(E,\mathcal E)$-valued random variable on $(\Omega,\mathcal A,\operatorname P)$ with $X\sim\mu$
- $Y$ be an $(E,\mathcal E)$-valued random variable on $(\Omega,\mathcal A,\operatorname P)$ with$^1$ $(X,Y)\sim\mu\otimes Q$
Note that $$\xi:=\frac{p(Y)q(Y,X)}{p(X)q(X,Y)}$$ is almost surely well-defined. How can we show that $\operatorname E\left[\xi\right]=1$?
Let $$B:=\left\{(x,y)\in E^2:p(x)q(x,y)>0\right\}$$ and $N:=E^2\setminus B$. Note that $N$ is a $\mu\otimes Q$-null set and
\begin{equation} \begin{split} \operatorname E\left[\xi\right]&=\int\mu({\rm d}x)\int Q(x,{\rm d}y)1_B(x,y)\frac{p(y)q(y,x)}{p(x)q(x,y)}\\&=\int\lambda({\rm d}x)\lambda({\rm d}y)1_B(x,y)\tilde p(y)q(y,x)\\&=\int\mu({\rm d}y)\int Q(y,{\rm d}x)1_B(x,y). \end{split}\tag1 \end{equation}
However, $(1)$ is not equal to $1$ (unless there is some kind of "reversibility" allowing us to swap the arguments of $1_B$). So, is the claim wrong as stated?
The claim can be found inside the proof of Theorem 1 on page 13 here: https://arxiv.org/pdf/1810.07151.pdf. (The proof itself is too complicated. I guess the author missed the point that $2(a\wedge b)=a+b-|a-b|$ for all $a,b\in\mathbb R$.)
EDIT: If the claim is wrong, what I really want to show is the claim about the total variation distance in Theorem 1.
$^1$ see https://en.wikipedia.org/wiki/Transition_kernel#Product_of_kernels.