On Wednesday, July 18, 2018 at 2:00:47 AM UTC, [email protected] wrote:
>
>  
> On Tuesday, July 17, 2018 at 12:00:08 PM UTC, Bruno Marchal wrote:
>>
>>
>> On 16 Jul 2018, at 23:08, [email protected] wrote:
>>
>>
>>
>> On Monday, July 16, 2018 at 8:30:58 AM UTC-6, Bruno Marchal wrote:
>>>
>>>
>>> On 13 Jul 2018, at 01:55, [email protected] wrote:
>>>
>>>
>>>
>>> On Wednesday, July 11, 2018 at 2:16:24 PM UTC-6, [email protected] 
>>> wrote:
>>>>
>>>>
>>>>
>>>> On Tuesday, July 10, 2018 at 4:42:44 PM UTC-6, Brent wrote:
>>>>>
>>>>>
>>>>>
>>>>> On 7/10/2018 3:01 PM, [email protected] wrote:
>>>>>
>>>>> *IIRC, the above quote is also in the Wiki article. It's not a 
>>>>> coherent argument; not even an argument but an ASSERTION. Let's raise the 
>>>>> level of discourse. It says we always get a or b, no intermediate result 
>>>>> when the system is in a superposition of states A and B.. Nothing new 
>>>>> here. 
>>>>> Key question: why does this imply the system is in states A and B 
>>>>> SIMULTANEOUSLY before the measurement? AG  *
>>>>>
>>>>>
>>>>> Because, in theory and in some cases in practice, there is a direct 
>>>>> measurement of the superposition state, call it C, such that you can 
>>>>> directly measure C and always get c, but when you have measured and 
>>>>> confirmed the system is in state c and then you measure A/B you get a or 
>>>>> b 
>>>>> at random.   The easiest example is SG measurements of sliver atom spin 
>>>>> orientation where spin UP can be measured left/right and get a LEFT or a 
>>>>> RIGHT at random, but it can be measured up/down and you always get UP.  
>>>>> Any 
>>>>> particular  orientation can be *written* as a superposition of two 
>>>>> orthogonal states.  
>>>>>
>>>>
>>>> *When you're trying to explain esoteric issues to a moron in physics, 
>>>> you need to be more explicit. These are the issues that cause confusion 
>>>> and 
>>>> caused me to fail to "get it". After some subsequent posts, you seem to be 
>>>> saying that in an SG spin experiment where the measurement base is UP/DN, 
>>>> the system being measured is ALSO in a superposed LEFT/RIGHT state which 
>>>> is 
>>>> also measured (by an SG device designed to measure spin?), and that the 
>>>> LEFT/RIGHT superposed state persists with some persistent eigenvalue after 
>>>> UP/DN is measured. It's murky for us morons.  How does one get the system 
>>>> to be measured in a superposition of RIGHT/LEFT; what is the operator for 
>>>> which that superposition is an eigenstate, and what is the value of the 
>>>> persistent eigenvalue?*
>>>>
>>>> *Furthermore, you finally assert that since the RIGHT/LEFT state 
>>>> persists -- meaning that particle is in some DEFINITE state after the spin 
>>>> is measured -- and since (as you finally, finally assert) that that state 
>>>> can be written as a superposition of UP/DN, all is well -- in the sense 
>>>> that we can now be certain that the system is physically and 
>>>> simultaneously 
>>>> in the UP and DN states (which I am claiming is a fallacy). *
>>>>
>>>> *HOWEVER, assuming that I understand your argument after filing the 
>>>> gaps in your presentation (and pointing to some unanswered issues), I now 
>>>> must "rant" again that the UP/DN superposed representation is NOT unique. 
>>>> Thus, since there are finitely many or uncountable many such 
>>>> representations, and since (as per LC) QM has no preferred basis, your 
>>>> argument for the physical simultaneity of UP and DN states fails. I mean, 
>>>> I 
>>>> could write the superposed states in the basis (UP + DN) and (UP - DN), or 
>>>> in many other bases. Absent uniqueness of bases, one cannot assert that 
>>>> the 
>>>> system is physically and simultaneously in any particular pair of basis 
>>>> vectors.*
>>>>
>>>> *AG*
>>>>
>>>
>>> *I've been looking over your references to Peres. CMIIAW, but AFAICT he 
>>> doesn't deal with the issue I have been "ranting" about; namely, the 
>>> non-uniqueness of bases, implying IMO that the concept of simultaneous 
>>> physical states of the components of a superposition is an additional, 
>>> unsupported assumption of QM which leads to some popular misconceptions of 
>>> what QM is telling us. *
>>>
>>>
>>>
>>> Then you need to find a new explanation of the interference that occurs 
>>> in basically all quantum experiments, like the two slits, the statistics of 
>>> results with Stern-Gerlach spin measuring apparatus, etc.
>>>
>>
>> *I am not trying to explain the interference. *
>>
>>
>> You should. That is the whole problem. How can we get interference if the 
>> wave describes only our knowledge state. The reason why we consider the 
>> wave physically real is that the wave interfere, even the wave associate to 
>> a single particle. 
>>
>>
>>
>> *Rather I am pointing out an unnecessary assumption that leads to 
>> paradoxes.*
>>
>>
>> ?
>>
>>
>>
>>
>> * See comment below. AG*
>>  
>>
>>> The whole point of the physical wave amplitudes is that the diverse 
>>> superposed components have a physical role, through destructive or 
>>> constructive, or in between, interference.
>>>
>>
>> *The amplitudes give probabilities of occurrence, confirmed by 
>> measurements. Nothing more. You forget that the components of the 
>> superposition are usually assumed to be orthogonal states, which don't 
>> mutually interfere. Thus, you are claiming to explain interference from 
>> component states which don't interfere. *
>>
>>
>> That is what we do with any wave, and there is no problem there. It just 
>> that cos(pi/2) is zero.
>>
>
*You're mistaken. In quantum superpositions, orthogonal does not mean 90 
deg out of phase -- as is the case for ordinary vectors in the plane -- but 
that the inner product is zero. Hence, since the inner product of all 
components of a superposition are mutually orthogonal, or zero, how can you 
claim that interference exists? AG*
 

> The problem here is that the amplitude of the wave, when squared, give a 
>> probability to find a particle somewhere, but this forced us to make the 
>> wave physical, as it will behave differently if there is two slits, one 
>> splits, etc. 
>>
>>
>>
>>
>>
>> *Try this; in the case of radioactive decay, can you define the 
>> interference between Decayed and Undecayed states? AG*
>>
>>
>> It is not relevant. I prefer ro use superposition of spin, than a 
>> temporal phenomenon. 
>>
>
> *OK, then use superposition of spin and describe the interference. Note 
> that since the Up and Dn are orthogonal, there is no interference. That is, 
> generally, when we write a superposition where the components are 
> eigenstates, it is assumed the components are mutually orthogonal, hence no 
> interference. AG*
>
>>  
>>
>>> Note that the discussion here supposed the quantum theory, but you are 
>>> free of course to propose an alternative. Many have tried without success, 
>>> though.
>>>
>>
>> *What I am doing is asking the usual suspects the basis for the 
>> assumption that the components of a superposition physically exist 
>> simultaneously. So far, IMO, their silence is pregnant. They can't. AG *
>>
>>
>>
>> Then explain me what happens in the two slit experiments, when we send 
>> the particles “one by one”.
>> You need superposition to explain this. It is the base of QM: particles 
>> dynamics are described by waves, and those wave do superpose and interfere, 
>> even when the particles are alone. 
>>
>
> *I don't have to explain everything, and in fact I cannot. All I want to 
> know is how can there be interference among components of a superposition, 
> when they are mutually orthogonal. AG *
>
>>
>> Bruno
>>
>>
>>
>>
>>
>>
>>> Bruno
>>>
>>>
>>>
>>>
>>>
>>> *Incidentally, when you earlier referred to a RIGHT/LEFT superposition, 
>>> did you mean circular polarization, or right and left directions in a SG 
>>> apparatus in relation to Up/Dn measurements? TIA, AG * 
>>>
>>>>
>>>>> This is true in general.  Any state can be written as a superposition 
>>>>> of states in some other basis.  But it is not generally true that we can 
>>>>> prepare or directly measure a system in any given state.  So those states 
>>>>> we can't directly access, we tend to think of them as existing only as 
>>>>> superpositions of states we can prepare.
>>>>>
>>>>> Brent
>>>>>
>>>>
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