> On 30 Oct 2018, at 14:21, [email protected] wrote:
> 
> 
> 
> On Tuesday, October 30, 2018 at 8:58:30 AM UTC, Bruno Marchal wrote:
> 
>> On 29 Oct 2018, at 13:55, [email protected] <javascript:> wrote:
>> 
>> 
>> 
>> On Monday, October 29, 2018 at 10:22:02 AM UTC, Bruno Marchal wrote:
>> 
>>> On 28 Oct 2018, at 13:21, [email protected] <> wrote:
>>> 
>>> 
>>> 
>>> On Sunday, October 28, 2018 at 9:27:56 AM UTC, Bruno Marchal wrote:
>>> 
>>>> On 25 Oct 2018, at 17:12, [email protected] <> wrote:
>>>> 
>>>> 
>>>> 
>>>> On Tuesday, October 23, 2018 at 10:39:11 PM UTC, [email protected] 
>>>> <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.



> So if we're measuring spin, the result will always be an eigenstate of the 
> spin vector for phi1 or phi2. But (up + down) and (up - down) are NOT 
> eigenstates of either. How then can you justify your claim of measuring (up + 
> down) or (up - down)? AG  


By rotating the polariser filter: (abstracting from some normalising factor 
which is supposed to be 1/sqrt(2))

up’ = up + down
down’ = up - down

up = up’ + down’
down = up’ - down’

If you measure a set of photons all in the state up’= up+down in the base {up’, 
down’}, they all get the same result up'.
If you measure a set of photons from a mixture of up and down, in the same base 
{up’, down’}, half of them will be up’, and half of them will be down’.

Bruno






> 
>> Buy the book by David Albert. It will help you a lot, I think.
>> 
>> Bruno
>> 
>> 
>> 
>> 
>> 
>>> 
>>> Bruno
>>> 
>>> 
>>> 
>>> 
>>> 
>>>> 
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