Take the random sample $X_1, \dots, X_n$ with mean $\mu$ and variance $\sigma^2 < \infty$. Now assume the $X_i$ are Poisson random variables with parameter $\lambda$. I am told that the Lehmann-Scheffè theorem directly implies the identity $E[S^2 \mid \bar{X}] = \bar{X}$, where $S^2 = \dfrac{1}{n - 1} \sum_{i = 1}^n \left( X_i - \bar{X} \right)^2$ and $\bar{X} = \dfrac{1}{n} \sum_{i = 1}^n X_i$. And when I say 'directly', I mean in the sense that there is no derivation necessary (I already know that it can be derived, so that's not the part I'm interested in). I would like to see how this is so.
I am currently studying the textbook All of Statistics: A Concise Course in Statistical Inference by Larry Wasserman. From what I can tell, there (surprisingly!) is no mention of Lehmann-Scheffè in this textbook (I also checked the index).
Furthermore, the Wikipedia page for Lehmann-Scheffè also isn't clear on this.
So how exactly does the Lehmann-Scheffè theorem directly imply the identity $E[S^2 \mid \bar{X}] = \bar{X}$?