If we have state $\lvert\psi\rangle \in (\mathbb{C}^{2})^{\otimes n}$ in an $\textit{n}$-qubit system with Pauli operators $P$ such that $P \in \{I, X, Y, Z\}^{n}$, how can we design a circuit/procedure using multiple circuits and/or classical processing that would output a real output $\alpha$ which is on average equal to $$ Tr((P_{1} \otimes ... \otimes P_{n})\lvert \psi \rangle \langle \psi \rvert) $$
Maybe as a start, say our possible outcomes are $x \in \{0, 1\}^{n}$, so that when we measure an individual qubit $j$ of $\lvert \psi \rangle$ with projections $\{P_{j, 0}, P_{j, 1}\}$ we get an outcome $x_{i} \in \{0/1\}$. Can we obtain outcomes $x_{1},...,x_{n}$ simultaneously and what is the probability of obtaining those outcomes simultaneously? If I'm understanding observables correctly, the observable for this system would be $$O = \sum\limits_{i \in \{I, X, Y, Z\}^{n}} \sum\limits_{j \in \{0, 1\}} x_{j} P_{i, j}$$ although I'm not 100% sure if that's relevant to the problem.