On Tuesday, April 24, 2018 at 1:24:14 AM UTC, Bruce wrote:
>
> From: <[email protected] <javascript:>>
>
> On Tuesday, April 24, 2018 at 12:14:06 AM UTC, [email protected] wrote: 
>>
>>
>> On Monday, April 23, 2018 at 11:54:15 PM UTC, Bruce wrote: 
>>>
>>> From: <[email protected]>
>>>
>>> On Monday, April 23, 2018 at 7:38:30 PM UTC, [email protected] wrote: 
>>>
>>>> On Monday, April 23, 2018 at 1:20:05 PM UTC, [email protected] 
>>>> wrote: 
>>>>>
>>>>>
>>>>>
>>>>> On Monday, April 23, 2018 at 8:58:53 AM UTC, Bruce wrote: 
>>>>>>
>>>>>> From: <[email protected]>
>>>>>>
>>>>>>
>>>>>> On Monday, April 23, 2018 at 5:53:59 AM UTC, Bruce wrote: 
>>>>>>>
>>>>>>> From: <[email protected]>
>>>>>>>
>>>>>>>
>>>>>>> Let's agree that electrons A and B form a singlet entangled system. 
>>>>>>> Let's further agree that they are non separable. What do you do with 
>>>>>>> the 
>>>>>>> fact that when their spins are measured, they ARE in different spatial 
>>>>>>> locations, not even space separated in Bell experiments. How do we deal 
>>>>>>> with this FACT? AG
>>>>>>>
>>>>>>>
>>>>>>> What do you want me to do with the fact? I learn to live with facts 
>>>>>>> that I can't do anything about. The fact that the system is non-local 
>>>>>>> is a 
>>>>>>> fact that you just have to come to terms with.
>>>>>>>
>>>>>>> Bruce
>>>>>>>
>>>>>>
>>>>>> *ISTM that when you have a theory that seems correct and in some 
>>>>>> sense is well tested, but there are facts which contradict it, in this 
>>>>>> case 
>>>>>> a key fact right in front of your nose which contradicts it -- the fact 
>>>>>> that we see as plain as daylight that the subsystems as spatially 
>>>>>> separated 
>>>>>> -- invariably the theory must be wrong. AG*
>>>>>>
>>>>>>
>>>>>> I wish you luck with your project to prove quantum mechanics wrong.
>>>>>>
>>>>>> Bruce
>>>>>>
>>>>>
>>>>> *Right now I have a more modest goal. Starting from the postulates of 
>>>>> QM, how do you justify writing the wf of the singlet state as a 
>>>>> superposition of tensor product states? TIA AG *
>>>>>
>>>>
>>>> *What it's not. It's not the SWE. It's not Born's Rule. It's not the 
>>>> operator correspondence with observables. AG *
>>>>
>>>
>>> *I suppose it could be traced to the superposition principle; that the 
>>> state vector of the singlet state is a linear combination of the states 
>>> which are members of the corresponding Hilbert space of the system. But why 
>>> are these states tensor product states? AG*
>>>
>>>
>>> Why try worrying these things out for yourself? The easiest thing is to 
>>> go and look up a text book.
>>>
>>> Bruce
>>>
>>
>> *Recall when I asked whether entanglement necessarily implies non 
>> locality. You replied "not necessarily" and gave the classical example of 
>> elastic scattering of billiard balls where the momentum of its constituents 
>> and the whole system is known exactly. No uncertainty. In the wf for the 
>> singlet system you assume a definite net spin angular momentum, zero. How 
>> can you treat the singlet system quantum mechanically and at the same time 
>> assume you know its spin momentum exactly? Do you think this question could 
>> be answered in a text book? How could I even pose it to an inert, non 
>> responsive medium? AG *
>>
>
> *I just took a quick look at chapter 15, section 4 of Merzbacher, Quantum 
> Mechanics (Third Edition). The tensor equation can't be copied. It appears 
> in the blank lines below. Immediately you can see the problem with this 
> kind of treatment. It doesn't explain WHY, from First Principles, the 
> tensor product can be used to describe the composite system. It's virtually 
> impossible to find an explanation from First Principles. AG*
>
>
>  4. Quantum Dynamics in Direct Product Spaces and Multiparticle Systems. 
> Often the state vector space of a system can be regarded as the direct, 
> outer, or tensor product of vector spaces for simpler subsystems. The 
> direct product space is formed from two independent unrelated vector spaces 
> that are respectively spanned by the basis vectors /A;) and I B;) by 
> constructing the basis vectors 
>
> Although the symbol @ is the accepted mathematical notation for the direct 
> product of state vectors, it is usually dispensed with in the physics 
> literature, and we adopt this practice when it is unlikely to lead to 
> misunderstandings. If n1 and n2 are the dimensions of the two factor 
> spaces, the product space has dimension nl X n2. This idea is easily 
> extended to the construction of direct product spaces from three or more 
> simple spaces.
>
>
> Quite right. And what else are you going to use  for many-particle systems 
> that have independent Hilbert spaces -- you multiply them together, of 
> course.
>
> Bruce
>

Is this what you would characterize as a rigorous analysis? I can think of 
other alternatives. The answer has to be from First Principles or it's just 
hand waving. AG

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