> On 8 Nov 2018, at 18:25, agrayson2...@gmail.com wrote:
> 
> 
> 
> On Thursday, November 8, 2018 at 11:04:20 AM UTC, Bruno Marchal wrote:
> 
>> On 6 Nov 2018, at 12:22, agrays...@gmail.com <javascript:> wrote:
>> 
>> 
>> 
>> On Tuesday, November 6, 2018 at 9:27:31 AM UTC, Bruno Marchal wrote:
>> 
>>> On 4 Nov 2018, at 22:02, agrays...@gmail.com <> wrote:
>>> 
>>> 
>>> 
>>> On Sunday, November 4, 2018 at 8:33:10 PM UTC, jessem wrote:
>>> 
>>> 
>>> On Wed, Oct 31, 2018 at 7:30 AM Bruno Marchal <mar...@ulb.ac.be <>> wrote:
>>> 
>>>> On 30 Oct 2018, at 14:21, agrays...@gmail.com <> wrote:
>>>> 
>>>> 
>>>> 
>>>> On Tuesday, October 30, 2018 at 8:58:30 AM UTC, Bruno Marchal wrote:
>>>> 
>>>>> On 29 Oct 2018, at 13:55, agrays...@gmail.com <> wrote:
>>>>> 
>>>>> 
>>>>> 
>>>>> On Monday, October 29, 2018 at 10:22:02 AM UTC, Bruno Marchal wrote:
>>>>> 
>>>>>> On 28 Oct 2018, at 13:21, agrays...@gmail.com <> wrote:
>>>>>> 
>>>>>> 
>>>>>> 
>>>>>> On Sunday, October 28, 2018 at 9:27:56 AM UTC, Bruno Marchal wrote:
>>>>>> 
>>>>>>> On 25 Oct 2018, at 17:12, agrays...@gmail.com <> wrote:
>>>>>>> 
>>>>>>> 
>>>>>>> 
>>>>>>> On Tuesday, October 23, 2018 at 10:39:11 PM UTC, agrays...@gmail.com 
>>>>>>> <http://gmail.com/> wrote:
>>>>>>> If a system is in a superposition of states, whatever value measured, 
>>>>>>> will be repeated if the same system is repeatedly measured.  But what 
>>>>>>> happens if the system is in a mixed state? TIA, AG
>>>>>>> 
>>>>>>> If you think about it, whatever value you get on a single trial for a 
>>>>>>> mixed state, repeated on the same system, will result in the same value 
>>>>>>> measured repeatedly. If this is true, how does measurement distinguish 
>>>>>>> superposition of states, with mixed states? AG
>>>>>> 
>>>>>> That is not correct. You can distinguish a mixture of particles in the 
>>>>>> up or down states with a set of 1/sqrt(2)(up+down) by measuring them 
>>>>>> with the {1/sqrt(2)(up+down), 1/sqrt(2)(up-down}) discriminating 
>>>>>> apparatus. With the mixture, half the particles will be defected in one 
>>>>>> direction, with the pure state, they will all pass in the same 
>>>>>> direction. Superposition would not have been discovered if that was not 
>>>>>> the case.
>>>>>> 
>>>>>> And someone will supply the apparatus measuring (up + down), and (up - 
>>>>>> down)? No such apparatuses are possible since those states are 
>>>>>> inherently contradictory. We can only measure up / down. AG
>>>>> 
>>>>> You can do the experience by yourself using a simple crystal of calcium 
>>>>> (CaCO3, Island Spath), or with polarising glass. Or with Stern-Gerlach 
>>>>> devices and electron spin. Just rotating (90° or 180°) an app/down 
>>>>> apparatus, gives you an (up + down)/(up - down) apparatus. 
>>>>> 
>>>>> I don't understand. With SG one can change the up/down axis by rotation, 
>>>>> but that doesn't result in an (up + down), or (up - down) measurement. If 
>>>>> that were the case, what is the operator for which those states are 
>>>>> eigenstates? Which book by Albert? AG
>>>> 
>>>> David Z Albert, Quantum Mechanics and Experience, Harvard University 
>>>> Press, 1992.
>>>> https://www.amazon.com/Quantum-Mechanics-Experience-David-Albert/dp/0674741137
>>>>  
>>>> <https://www.amazon.com/Quantum-Mechanics-Experience-David-Albert/dp/0674741137>
>>>> 
>>>> Another very good books is
>>>> 
>>>> D’Espagnat B. Conceptual foundations of Quantum mechanics,  I see there is 
>>>> a new edition here:
>>>> https://www.amazon.com/Conceptual-Foundations-Quantum-Mechanics-Advanced/dp/0738201049/ref=sr_1_1?s=books&ie=UTF8&qid=1540889778&sr=1-1&keywords=d%27espagnat+conceptual+foundation+of+quantum+mechanics&dpID=41NcluHD6fL&preST=_SY291_BO1,204,203,200_QL40_&dpSrc=srch
>>>>  
>>>> <https://www.amazon.com/Conceptual-Foundations-Quantum-Mechanics-Advanced/dp/0738201049/ref=sr_1_1?s=books&ie=UTF8&qid=1540889778&sr=1-1&keywords=d%27espagnat+conceptual+foundation+of+quantum+mechanics&dpID=41NcluHD6fL&preST=_SY291_BO1,204,203,200_QL40_&dpSrc=srch>
>>>> 
>>>> It explains very well the difference between mixtures and pure states.
>>>> 
>>>> Bruno
>>>> 
>>>> Thanks for the references. I think I have a reasonable decent 
>>>> understanding of mixed states. Say a system is in a mixed state of phi1 
>>>> and phi2 with some probability for each. IIUC, a measurement will always 
>>>> result in an eigenstate of either phi1 or phi2 (with relative 
>>>> probabilities applying).
>>> 
>>> If the measurement is done with a phi1/phi2 discriminating apparatus. Keep 
>>> in mind that any state can be seen as a superposition of other oblique or 
>>> orthogonal states.
>>> 
>>> I don't know if you're restricting the definition of phi1 and phi2 to some 
>>> particular type of eigenstate or not, but in general aren't there pure 
>>> states that are not eigenstates of any physically possible measurement 
>>> apparatus, so there is no way to directly measure that a system is in such 
>>> a state?
>>> 
>>> Yes, such states exist IIUC. That's why I don't understand Bruno's claim 
>>> that Up + Dn and Up - Dn can be measured with any apparatus,
>> 
>> Not *any*¨apparatus, but a precise one, which in this case is the same 
>> apparatus than for up and down, except that it has been rotated.
>> 
>> 
>> 
>> 
>>> since they're not eigenstates of the spin operator, or any operator.
>> 
>> This is were you are wrong. That are eigenstates of the spin operator when 
>> measured in some direction.
>> 
>> If what you claim is true, then write down the operator for which up + dn 
>> (or up - dn) is an eigenstate? AG 
> 
> 
> It is the operator corresponding to the same device, just rotated from pi/2, 
> or pi (it is different for spin and photon). When I have more time, I might 
> do the calculation, but this is rather elementary quantum mechanics. (I am 
> ultra-busy up to the 15 November, sorry). It will have the same shape as the 
> one for up and down, in the base up’ and down’, so if you know a bit of 
> linear algebra, you should be able to do it by yourself.
> 
> Bruno
> 
> You don't have to do any calculation. Just write down the operator which, you 
> allege, has up + dn or up - dn as an eigenstate. I don't think you can do it, 
> because IMO it doesn't exist. AG 


If up and down are represented by the column (1 0) and (0 1) the corresponding 
observable is given by the diagonal matrix 

1  0
0 -1

Then the up’ = 1/sqrt(2) (1 1), and down’ = 1/sqrt(2) (1 -1),

So the operator, written in the base up down, will be 

0 1
1 0

 Here the eigenvalue +1 and -1 correspond to up (up’) or down (down’).

I have no clue why you think that such operator would not exist. All pure state 
can be seen as a superposition, in the rotated base, and you can always build 
an operator having them as eigenvalues.

Bruno






> 
>  
> 
> 
> 
> 
> 
>> 
>> Julian Swinger (and Townsend) showed that the formalism of (discrete, spin, 
>> qubit) quantum mechanics is derivable from 4 Stern-Gerlach experiments, 
>> using only real numbers, but for a last fifth one, you need the complex 
>> amplitudes, and you get the whole core of the formalism.
>> 
>> Bruno
>> 
>> 
>> 
>> 
>>> Do you understand Bruno's argument in a previous post on this topic? AG 
>>> 
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