On Tue, Jul 31, 2018 at 1:11 AM Brent Meeker <[email protected]> wrote:

>
>
> On 7/30/2018 9:21 PM, [email protected] wrote:
>
>
>
> On Tuesday, July 31, 2018 at 1:34:58 AM UTC, Brent wrote:
>>
>>
>>
>> On 7/30/2018 4:40 PM, [email protected] wrote:
>>
>>
>>
>> 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. *
>
>
> 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.
>
> *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.
>
>

What if the cat is on Pluto for this one hour?  Would it not be perfectly
isolated from us on Earth, and thus remain in a superposition until the the
several hours it takes for light to get to Earth from Pluto reaches us?

Jason

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