Alice's outcome is random. Conditional on knowing it, Bob may assign a different quantum state, but without that classical record he sees the same density matrix. For the displayed pure two-qubit state, his reduced density matrix before Alice's measurement is
After Alice's computational-basis measurement with the outcome unannounced, the weighted mixture is exactly this same matrix. More generally, for any local trace-preserving operation with measurement operators ,
The equality follows from the cyclic property of the partial trace for operators acting on Alice's subsystem. Bob's every local outcome probability therefore remains unchanged. This is the no-communication theorem: . Conditional state changes become usable correlations only when the classical outcomes are compared.

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