- 24,488
- 15,057
True, but you cannot treat the Geiger counter by solving the Schrödinger wave equation exactly for its ##10^{30}## (or so) constituents, and it is indeed completely sufficient to treat the relevant physics of the Geiger counter in terms of classical physics. It's misleading to write ##|\text{decay measured} \rangle## since the observation that a decay has been registered is not a microscopic but a macrscopic observable. Here lies the key for the understanding that there is no measurement problem, and this was emphasized already by Bohr in the early days of QT.
To understand theoretically, why the classical description of the macroscopic observables of macroscopic systems is a valid approximation of QT, you need quantum statistics or "many-body theory". That's all I'm saying.
To understand theoretically, why the classical description of the macroscopic observables of macroscopic systems is a valid approximation of QT, you need quantum statistics or "many-body theory". That's all I'm saying.