> On 10 Nov 2018, at 01:27, [email protected] wrote:
> 
> 
> 
> On Friday, November 9, 2018 at 12:26:52 PM UTC, Bruno Marchal wrote:
> 
>> On 8 Nov 2018, at 18:25, [email protected] <javascript:> wrote:
>> 
>> 
>> 
>> On Thursday, November 8, 2018 at 11:04:20 AM UTC, Bruno Marchal wrote:
>> 
>>> On 6 Nov 2018, at 12:22, [email protected] <> wrote:
>>> 
>>> 
>>> 
>>> On Tuesday, November 6, 2018 at 9:27:31 AM UTC, Bruno Marchal wrote:
>>> 
>>>> On 4 Nov 2018, at 22:02, [email protected] <> 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 <[email protected] <>> wrote:
>>>> 
>>>>> 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] <> 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.
>>>> 
>>>> 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.
> 
> Because the measured spin state is Up or Dn along some axis, never anything 
> in between. Up + Dn or Up - Dn is not physically realizable in unprimed 
> basis. AG


If the measured spin state is Up or Dn along some axis, the measured spin state 
will be Up + Dn or Up - Down along the axis obtained by rotating the measuring 
apparatus adequately. That is physically realisable with spin (by just rotating 
the Stern-Gerlach apparatus) of with light polarisation (rotating the polariser 
or the CaCO3 crystal).

Bruno




> 
> 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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