On Sunday, November 11, 2018 at 5:43:00 PM UTC, [email protected] wrote:
>
>
>
> On Sunday, November 11, 2018 at 7:52:00 AM UTC, Bruno Marchal wrote:
>>
>>
>> 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] 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, agrays...@
>>>>>>>>>> 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
>>>>>>>>
>>>>>>>> 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
>>>>>>>>
>>>>>>>> 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. 
>>
>
> *You are mistaken. According to QM, the measured value is always an 
> eigenvalue of one of the eigenstates of the operator, in this case either 
> Up or Dn. After the measurement, the system is in the eigenstate 
> corresponding to the eigenvalue measured. This eigenstate can be written in 
> many different bases, but this does not change what has been MEASURED. If 
> you rotate the apparatus, the same exact situation exists. You will NEVER 
> measure Up + Dn or Up - Dn regardless of how the apparatus is oriented. AG*
>

*Important correction; before measurement, say of spin, the wf can be 
written in many forms, one being a linear combination of the eigenstates Up 
and Dn. It's never measured in states Up + Dn or Up - Dn, since these are 
not eigenstates of the spin operator. This is basic QM. Just because there 
are many ways to express a wf, doesn't mean a measurement measures every 
possible expression of that state. AG*

>
> 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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>>>>>
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