On Wednesday, January 15, 2025 at 5:15:35 PM UTC-7 Brent Meeker wrote:




On 1/15/2025 1:39 PM, Russell Standish wrote:

What you are talking about is known as the preferred basis problem. This 
has been discussed on this list before. My own take on this is that you 
can't ignore the observer. In any physical situation, an observer chooses 
some measurement apparatus (thereafter you can sweep the observer under the 
carpet, and focus on the measurement apparatus). The measurement apparatus 
entangled with the system under question has the dynamics that tensor 
product of measuring apparatus state with that of the system evolves to be 
diagonal in some basis, aka "einselection". And that is the origin of the 
preferred basis. In the multiverse, there will also be other observers 
choosing different apparati eg ones that select a complementary basis (eg 
momentum where the first chooses to measure position). These will have a 
different set of preferred basis. There is only a problem if you try to 
ignore the existence of observers and measuring devices. Cheers On Wed, Jan 
15, 2025 at 11:58:33AM -0800, Alan Grayson wrote: 

It's easy to show that a Superposition does NOT imply that a system 
represented by a linear sum of a pure set of basis vectors, is in all of 
those states simultaneusly.This follows from the fact that the WF is an 
element of a vector space, a Hilbert space, and in vector spaces there is 
no unique set of basis vectors. IOW, any set of basis vectors can represent 
the WF of a system, and if we claim the system is in all states of some 
superposition, it must also be in all states of any other superposition. 

If it's in a pure state then that is single vector in Hilbert space.  So 
there is a basis 
that includes that vector and then the state has a single component in that 
basis.
Of course there is no way to measure in that basis without already knowing 
what 
what it is.

Brent

 
 Generally speaking, isn't a superposition a linear sum of pure states? AG


And every set of basis vectors is equivalent to, and indistinguishable from 
any other set of basis vectors. This shows that Schrodinger could have 
denied the usual interpretation of the WF as a superposition where the 
system it represented could be interpreted as being in all pure states in 
its sum simultaneously, without constructing his Cat experiment. He simply 
had to remind his colleagues that the set of basis vectors in a vector 
space is not unique. AG -- You received this message because you are 
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