On Thursday, October 24, 2019 at 12:56:29 PM UTC-6, Philip Thrift wrote:
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> On Thursday, October 24, 2019 at 9:27:14 AM UTC-5, Alan Grayson wrote:
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>> On Monday, October 21, 2019 at 6:21:26 PM UTC-6, Alan Grayson wrote:
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>>> On Monday, October 21, 2019 at 12:03:20 AM UTC-6, Brent wrote:
>>>>
>>>>
>>>> On 10/20/2019 10:46 PM, Alan Grayson wrote:
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>>>> On Sunday, October 20, 2019 at 6:35:10 PM UTC-6, Brent wrote:
>>>>>
>>>>>
>>>>> On 10/20/2019 4:58 PM, Alan Grayson wrote:
>>>>>
>>>>> On Sunday, October 20, 2019 at 11:35:13 AM UTC-6, Brent wrote:
>>>>>>
>>>>>>
>>>>>> On 10/19/2019 6:56 PM, Alan Grayson wrote:
>>>>>>
>>>>>> Sean says the decoherence time is 10^(-20) sec. So when the box is 
>>>>>>> closed, the cat is in a superposition of alive and dead during that 
>>>>>>> time 
>>>>>>> interval, assuming the decay hasn't happened. If that's the case, I 
>>>>>>> don't 
>>>>>>> see how decoherence solves the paradox, unless we can assume an initial 
>>>>>>> condition where the probability of one component of the superposition, 
>>>>>>> that 
>>>>>>> the cat is dead, is zero. Maybe this is the solution. What do you 
>>>>>>> think? AG
>>>>>>>
>>>>>>
>>>>>> Maybe this is an easier question; after decoherence, assuming the 
>>>>>> radioactive source hasn't decayed, what is the wf of the cat?  Is the 
>>>>>> cat 
>>>>>> in a mixed state, alive or dead with some probabIlity for each? AG
>>>>>>
>>>>>>
>>>>>> You can't "assume the radioactive source hasn't decayed".  The point 
>>>>>> Schroedinger's thought experiment is that when the box is closed you 
>>>>>> don't 
>>>>>> know whether or not it has decayed and so it is in a superposition of 
>>>>>> decayed and not-decayed and the cat is correlated with these states, so 
>>>>>> it 
>>>>>> is also in a superposition of dead and alive.
>>>>>>
>>>>>> Brent
>>>>>>
>>>>>
>>>>> I thought you might say this. OK, then what function does decoherence 
>>>>> have in possibly solving the apparent paradox of a cat alive and dead 
>>>>> simultaneously. TIA, AG 
>>>>>
>>>>>
>>>>> It doesn't necessarily solve "that problem".  Rather it shows why you 
>>>>> can never detect such a state, assuming you buy Zurek's idea of 
>>>>> envariance.  One way to look at it is it's the answer to Heisenberg's 
>>>>> question: Where is the cut between the quantum and the classical?  Once 
>>>>> envriance has acted, then the result is classical, i.e. you can ignore 
>>>>> the 
>>>>> other possibilities and renormalize the wave function.
>>>>>
>>>>> Brent
>>>>>
>>>>
>>>> Woudn't you agree that if the system, in the case a cat, goes classical 
>>>> after 10^(-20) sec, its state must be a mixture at that point in time even 
>>>> if the box hasn't been opened?  AG 
>>>>
>>>>
>>>> In MWI it's only a mixture FAPP.  But if you haven't opened the box 
>>>> (and Schroedinger was assuming an ideal box) you don't know whether the 
>>>> cat 
>>>> has "gone classical" or not.  So your representation of its state is still 
>>>> a superposition.  That's the QBist interpretation.  The wf is just what 
>>>> you 
>>>> know about the system.
>>>>
>>>
>>> Please remind me; if the wf is a *superposition* before the box is 
>>> opened, what exactly does this mean? That is, what does *interference* 
>>> mean in this circumstance? TIA, AG
>>>
>>
>> Please indulge me on this. At this point I have no clue what 
>> superposition and/or interference means in this context. TIA, AG 
>>
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> All these are couched in the vocabulary of the formulation and 
> interpretation of the theory one begins with, and so they have ambiguous 
> meanings.
>
> @philipthrift 
>

Can you answer the question assuming the CI? AG 

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