Thermal instabilities and noise modify quantum measurement statistics in a sensitive, nontrivial way across the weak-to-strong crossover depending on temperature, probe properties, and state selections.
By exact analogy, the negative displacement component (γ=ib−s/2) yields the same imaginary part, resulting in Tr( ˆP ρ−−) =P 0
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Weak-to-Strong Measurement Transition with Thermal Instabilities
Thermal instabilities and noise modify quantum measurement statistics in a sensitive, nontrivial way across the weak-to-strong crossover depending on temperature, probe properties, and state selections.