On Thursday, October 24, 2019 at 5:07:34 PM UTC-5, Alan Grayson wrote:
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> On Thursday, October 24, 2019 at 12:56:29 PM UTC-6, Philip Thrift wrote:
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>>
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>> On Thursday, October 24, 2019 at 9:27:14 AM UTC-5, Alan Grayson wrote:
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>>>
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>>> On Monday, October 21, 2019 at 6:21:26 PM UTC-6, Alan Grayson wrote:
>>>>
>>>>
>>>> On Monday, October 21, 2019 at 12:03:20 AM UTC-6, Brent wrote:
>>>>>
>>>>>
>>>>> On 10/20/2019 10:46 PM, Alan Grayson wrote:
>>>>>
>>>>> 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 
>>>
>>
>>
>> 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 
>



Just translate this into "CI", in whatever terms you like. It gives the 
same answers, so what difference does it make?

*The probability P for an event to occur is given by the square of the 
complex magnitude of a quantum amplitude for the event, Q. The quantum 
amplitude Q associated with an event is the sum of the amplitudes  
associated with every history leading to the event.*

[This] specifies how probabilities are to be computed. *This item builds 
the concept of superposition, and thus the possibility of quantum 
interference, directly into the formulation.* Specifying that the 
probability for an event is given as the magnitude-squared of a sum made 
from complex numbers, allows for negative, positive and intermediate 
interference effects. This part of the formulation thus builds the 
description of experiments such as the two-slit experiment directly into 
the formulation. A history is a sequence of fundamental processes leading 
to the the event in question. 

http://muchomas.lassp.cornell.edu/8.04/Lecs/lec_FeynmanDiagrams/node3.html 

@philipthrift

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