rkastner
- 264
- 38
My proposal has some affinity with this quote by Gisin, in the following sense: an offer wave (represented by |X>) is a physical possibility for property X to be actualized. However X can of course be decomposed into other properties (e.g., Yi) as Ʃi <Yi|X> |Yi>. The response by an absorber of adjoint property (confirmation wave) <X|Yi> <Yi| sets up an incipient transaction corresponding to that property, which may be actualized with the weight |<X|Yi>|^2 (i.e. probability).
This is the physical basis of von Neumann's 'Process 1' in which a pure state |X> transitions upon 'measurement' or 'observation' (in the usual parlance) into the mixed state
Ʃi |<X|Yi>|^2 |Yi><Yi|, with one of the |Yi><Yi| being randomly actualized as a property. Note that in this TI process, 'measurement' becomes precisely physically defined and is observer-independent. That problem is resolved by taking absorption (i.e., response of the absorber) into account.
If the intial |X> were responded to by adjoint <X| then that property would be actualized with certainty. However, since this is rarely the case, we don't have a classical type of realism. Also, it's not local wrt spacetime because of the advanced influences establishing the properties.
This is the physical basis of von Neumann's 'Process 1' in which a pure state |X> transitions upon 'measurement' or 'observation' (in the usual parlance) into the mixed state
Ʃi |<X|Yi>|^2 |Yi><Yi|, with one of the |Yi><Yi| being randomly actualized as a property. Note that in this TI process, 'measurement' becomes precisely physically defined and is observer-independent. That problem is resolved by taking absorption (i.e., response of the absorber) into account.
If the intial |X> were responded to by adjoint <X| then that property would be actualized with certainty. However, since this is rarely the case, we don't have a classical type of realism. Also, it's not local wrt spacetime because of the advanced influences establishing the properties.