On Sunday, June 24, 2018 at 3:03:07 AM UTC, Brent wrote:
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> On 6/23/2018 2:26 PM, [email protected] <javascript:> wrote:
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> On Saturday, June 23, 2018 at 9:21:05 PM UTC, [email protected] wrote: 
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>> On Saturday, June 23, 2018 at 7:52:08 PM UTC, Brent wrote: 
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>>> On 6/23/2018 12:02 AM, [email protected] wrote:
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>>> On Saturday, June 23, 2018 at 6:25:38 AM UTC, Brent wrote: 
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>>>> On 6/22/2018 3:13 PM, [email protected] wrote:
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>>>> *I've been struggling lately with how to interpret a superposition of 
>>>> states when it is ostensibly unintelligible, e.g., a cat alive and dead 
>>>> simultaneously, or a radioactive source decayed and undecayed 
>>>> simultaneously. If we go back to the vector space consisting of those 
>>>> "little pointing things", it follows that any vector which is a sum of 
>>>> other vectors, simultaneously shares the properties of the components in 
>>>> its sum. This is simple and obvious. I therefore surmise that since a 
>>>> Hilbert space is a linear vector space, this interpretation took hold as a 
>>>> natural interpretation of superpositions in quantum mechanics, and led to 
>>>> Schroedinger's cat paradox. I don't accept the explanation of decoherence 
>>>> theory, that we never see these unintelligible superpositions because of 
>>>> virtually instantaneous entanglements with the environment. Decoherence 
>>>> doesn't explain why certain bases are stable; others not, even though, 
>>>> apriori, all bases in a linear vector space are equivalent. These 
>>>> considerations lead me to the conclusion that a quantum superposition of 
>>>> states is just a calculational tool, and when the superposition consists 
>>>> of 
>>>> orthogonal component states, it allows us to calculate the probabilities 
>>>> of 
>>>> the measured system transitioning to the state of any component. In this 
>>>> interpretation, essentially the CI, there remains the unsolved problem of 
>>>> providing a mechanism for the transition from the SWE, to the collapse to 
>>>> one of the eigenfunctions when the the measurement occurs. I prefer to 
>>>> leave that as an unsolved problem, than accept the extravagance of the 
>>>> MWI, 
>>>> or decoherence theory, which IMO doesn't explain the paradoxes referred to 
>>>> above, but rather executes what amounts to a punt, claiming the paradoxes 
>>>> exist for short times so can be viewed as nonexistent, or solved. AG. *
>>>>
>>>>
>>>> If you're willing to take QM as simply a calculational tool, then QBism 
>>>> solve the problem of wf collapse.
>>>>
>>>> Brent
>>>>
>>>
>>> Thanks. I'll check it out. Is QBism a plausible theory? Do some 
>>> professional "heavies" accept it? AG 
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>>>
>>> Asher Peres started it and he was a "heavy weight".  Chris Fuchs has 
>>> been the main advocate, but he's kind of strange.  The interpretation is 
>>> not widely liked because it's the extreme end of instrumentalism.
>>>
>>> Brent
>>>
>>
>> *Let's go back to those little pointy things and write A = B + C, where B 
>> and C are basis states with appropriate multiplicative constants. Given 
>> this particular basis, one could interpret this equation as a superposition 
>> where A is understood as being in states B and C simultaneously. But A 
>> could be written in an infinite set of different sums using orthogonal or 
>> non orthogonal bases. So, given the lack of uniqueness, it seems an 
>> unwarranted stretch to assume any vector can be interpreted as being in two 
>> states simultaneously, If we drop this interpretation for quantum 
>> superpositions, most, possibly all the paradoxes go away. Who was the 
>> person who first interpreted a superposition in this way, which seems the 
>> root of many unnecessary, a[[ar problems in quantum mechanics? AG *
>>
>
> ... *Who first interpreted a quantum superposition this way, which seems 
> the root of many unnecessary, intractable problems in quantum mechanics, 
> inclusive of the idea that a particle can be in more than one position 
> simultaneously? AG*
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> Of course in theory any pure state can be taken to be a basis vector and 
> there is an operator for which that state is an eigenvector, i.e. a basis 
> in which it is not a superposition.  
>

*Can't any pure state be written as a superposition using another basis? AG*
 

> But in practice we don't know what that basis is and in general we cannot 
> physically realize the corresponding operator.  That's why a photon passing 
> thru Young's slits is said to be in a superposition of passing thru slit 1 
> and passing thru slit 2.  We know how to create an operator that measures 
> "passing thru slit 1" and we know how to create an operator that measures 
> "passing thru slit 2", but we don't know how to construct an operator that 
> measures "passes thru both slit 1 and slit 2".  We can write down the wf in 
> the basis of "passing thru slit 1" and "passing thru slit 2" and it's a 
> coherent sum, i.e. a superposition of those two.  Decoherence theory says 
> that we can't construct an instrument which will measure "passes thru both 
> slit 1 and slit 2" because such an instrument would quickly decohere into 
> one of the two stable states "passed thru 1" or "passed thru 2" and the 
> interference pattern would not form (in repeated trials).
>

*In Young's double slit experiment, IIUC we assume the wave goes through 
both slits simultaneously in order to model the interference after repeated 
trials.** But you say that's NOT what decoherence theory says. I find this 
baffling. In the seminal quantum experiment where one could, it seems, 
assume simultaneity of the component wf's, you say it's denied by 
decoherence theory. ** Maybe I missed the content of your comment. **In 
general I don't see the reason to assume simultaneity for components of a 
quantum superposition. How would you justify that interpretation of a 
quantum superposition? TIA, AG*
Brent

>

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