On Tuesday, July 31, 2018 at 6:11:18 AM UTC, Brent wrote:
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> On 7/30/2018 9:21 PM, agrays...@gmail.com <javascript:> wrote:
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> On Tuesday, July 31, 2018 at 1:34:58 AM UTC, Brent wrote: 
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>> On 7/30/2018 4:40 PM, agrays...@gmail.com wrote:
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>> On Monday, July 30, 2018 at 7:50:47 PM UTC, Brent wrote: 
>>>
>>>
>>>
>>> On 7/30/2018 8:02 AM, Bruno Marchal wrote:
>>>
>>> *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. *
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>
> Why is that problematic?  You must realize that the cat dying takes at 
> least several seconds, very long compared to decoherence times.  So the cat 
> is always in a *classical* state between |alive> and |dead>. These are 
> never in superposition. 
>


*When you start your analysis /experiment using decoherence theory, don't 
you assume the cat is isolated from the environment? It must be if you say 
it later decoheres (even if later is only a nano second). Why is this not a 
problem if, as you say, it is impossible to isolate the cat? AG *

>
> *It doesn't go away because the decoherence time is exceedingly short. *
>
>
> Yes is does go away.  Even light can't travel the length of a cat in a 
> nano-second.  
>
>
> *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 *
>
>
> It's not a fallacy.  It just doesn't apply to the cat or other macroscopic 
> objects, with rare laboratory exceptions. 
>

*Other than slit experiments where superposition can be interpreted as the 
system being in both component states simultaneously, why is this 
interpretation extendable to all isolated quantum systems? AG *

> Any old plane polarized photon can be represented as being in a 
> superposition of left and right circular polarization.  It is *not* the 
> case that a system is in all basis states at once unless you count being in 
> state *|x>*  with zero amplitude as being in *x*.
>
> Brent
>
>
>
>> Brent
>>
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