On Thursday, January 16, 2025 at 2:49:27 PM UTC-7 Brent Meeker wrote:




On 1/16/2025 3:04 AM, Alan Grayson wrote:



On Wednesday, January 15, 2025 at 6:51:28 PM UTC-7 Alan Grayson wrote:

On Wednesday, January 15, 2025 at 6:44:27 PM UTC-7 Brent Meeker wrote:




On 1/15/2025 4:55 PM, Alan Grayson wrote:



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


Right.  And a linear sum of vectors is a vector.

Brent


*If it can be proven what I've initially stated about a superposition, why 
is it necessary to consider entangement of experimenter and*
*apparatus, when the result follows directly from the properties of a 
vector space? AG* 


*Another question I have about superposition is this; if the wf for some 
system is written in a momentum basis, do other momentum bases *
*exist for expressing the wf? If so, is the set of momentum bases infinite? 
AG*



*It's Hilbert space.  For finite dimensions it's just a vector space.  
Forget about bases, vectors are things that at independent of bases.  Bases 
are arbitrary. Brent*


*Yes, of course, vectors are independent of bases, but I asked the question 
to determine if my conclusion about superposition, as described in the 
initial post on this thread, is correct.  For my conclusion to be true, for 
any wf representing a system as a superposition, there must be many bases 
which can also represent the same wf. So, for example, for a wf which can 
be expressed as a superposition of momentum states, are there other bases 
for which the same wf can be so expressed? I've never seen this done, and I 
wonder if it can be done. TY, AG*

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