On Tuesday, July 31, 2018 at 1:34:58 AM UTC, Brent wrote:
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> On 7/30/2018 4:40 PM, [email protected] <javascript:> wrote:
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> On Monday, July 30, 2018 at 7:50:47 PM UTC, Brent wrote: 
>>
>>
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>> On 7/30/2018 8:02 AM, Bruno Marchal wrote:
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>> *and claims the system being measured is physically in all eigenstates 
>> simultaneously before measurement.*
>>
>>
>>
>> Nobody claims that this is true. But most of us would I think agree that 
>> this is what happens if you describe the couple “observer particle” by QM, 
>> i.e by the quantum wave. It is a consequence of elementary quantum 
>> mechanics (unless of course you add the unintelligible collapse of the 
>> wave, which for me just means that QM is false). 
>>
>>
>> This talk of "being in eigenstates" is confused.  An eigenstate is 
>> relative to some operator.  The system can be in an eigenstate of an 
>> operator.  Ideal measurements are projection operators that leave the 
>> system in an eigenstate of that operator.  But ideal measurements are rare 
>> in QM.  All the measurements you're discussing in Young's slit examples are 
>> destructive measurements.  You can consider, as a mathematical convenience, 
>> using a complete set of commuting operators to define a set of eigenstates 
>> that will provide a basis...but remember that it's just mathematics, a 
>> certain choice of basis.  The system is always in just one state and the 
>> mathematics says there is some operator for which that is the eigenstate.  
>> But in general we don't know what that operator is and we have no way of 
>> physically implementing it.
>>
>> Brent
>>
>
> *I can only speak for myself, but when I write that a system in a 
> superposition of states is in all component states simultaneously, I am 
> assuming the existence of an operator with eigenstates that form a complete 
> set and basis, that the wf is written as a sum using this basis, and that 
> this representation corresponds to the state of the system before 
> measurement.  *
>
>
> In general you need a set of operators to have the eigenstates form a 
> complete basis...but OK.
>
> *I am also assuming that the interpretation of a quantum superposition is 
> that before measurement, the system is in all eigenstates simultaneously, 
> one of which represents the system after measurement. I do allow for 
> situations where we write a superposition as a sum of eigenstates even if 
> we don't know what the operator is, such as the Up + Dn state of a spin 
> particle. In the case of the cat, using the hypothesis of superposition I 
> argue against, we have two eigenstates, which if "occupied" by the system 
> simultaneously, implies the cat is alive and dead simultaneously. AG *
>
>
> Yes, you can write down the math for that.  But to realize that physically 
> would require that the cat be perfectly isolated and not even radiate IR 
> photons (c.f. C60 Bucky ball experiment).  So it is in fact impossible to 
> realize (which is why Schroedinger considered if absurd).
>


*CMIIAW, but as I have argued, in decoherence theory it is assumed the cat 
is initially isolated and decoheres in a fraction of a nano second. So, 
IMO, the problem with the interpretation of superposition remains. It 
doesn't go away because the decoherence time is exceedingly short. And for 
this reason I still conclude that Schroedinger correctly pointed out the 
fallacy in the standard interpretation of superposition; namely, that the 
system represented by a superposition, is in all components states 
simultaneously. AG *

>
> Brent
>
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