> On 18 Jul 2018, at 23:24, agrayson2...@gmail.com wrote:
> 
> 
> 
> On Wednesday, July 18, 2018 at 4:39:30 PM UTC, Bruno Marchal wrote:
> 
>> On 18 Jul 2018, at 05:02, agrays...@gmail.com <javascript:> wrote:
>> 
>> 
>> 
>> On Wednesday, July 18, 2018 at 2:00:47 AM UTC, agrays...@gmail.com 
>> <http://gmail.com/> wrote:
>>  
>> On Tuesday, July 17, 2018 at 12:00:08 PM UTC, Bruno Marchal wrote:
>> 
>>> On 16 Jul 2018, at 23:08, agrays...@gmail.com <> wrote:
>>> 
>>> 
>>> 
>>> On Monday, July 16, 2018 at 8:30:58 AM UTC-6, Bruno Marchal wrote:
>>> 
>>>> On 13 Jul 2018, at 01:55, agrays...@gmail.com <> wrote:
>>>> 
>>>> 
>>>> 
>>>> On Wednesday, July 11, 2018 at 2:16:24 PM UTC-6, agrays...@gmail.com 
>>>> <http://gmail.com/> wrote:
>>>> 
>>>> 
>>>> On Tuesday, July 10, 2018 at 4:42:44 PM UTC-6, Brent wrote:
>>>> 
>>>> 
>>>> On 7/10/2018 3:01 PM, agrays...@gmail.com <> 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.
> 
> 
> That is what I mean.
> 
> 
> 
> 
> 
>> Hence, since the inner product of all components of a superposition are 
>> mutually orthogonal, or zero, how can you claim that interference exists? AG
> 
> 
> A position (say at one hole) is models by a vector in an abstract linear 
> space. The position at the other hole (I’m thinking of the two slit 
> experiences) is represented by another vector. The fact that the two position 
> are distinct and distinguishable made them described by orthogonal vector in 
> that abstract linear space (an Hilbert space).
> 
> Orthogonal vectors don't manifest interference, as shown in the simple case 
> of vectors in a plane, which form a linear vector space. In the double slit 
> case, there IS interference of various types along the screen, the components 
> of the superposition DO interfere, but they are NOT orthogonal. AG  

That is a terrible wording. Let say that x is the state of the particle when 
going in slit x and y is the state in slit y. Interference comes from the fact 
that the particle can be in the state ax + by (with a^2 + b^2 = 1).





> 
>  
> The interference of statistics comes from the fact that the available stories 
> are described by a wave function, which describe my relative ignorance on 
> which histories I belong to. When the to holes are open, the particle state 
> might be described by a superposition of those two position, which makes some 
> angle different from PI/2,
> 
> The interference, constructive, destructive, or in between, depends on the 
> position of impacts and the distance between the slits. I don't deny 
> interference among the (two) component terms of the superposition in this 
> case.

OK.



> Rather, I object to the generalization of this idea to quantum superpositions 
> composed of orthogonal states. AG


You can use a non orthigal base, but the orthogonal one are more easy to 
handle, and can always been found (by a well known procedure).




>  
> so that interference terms can appear, and indeed can be reflected on the 
> screen by interference fringes if I repeat the experience with the same wave 
> again and again.
>  
> 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. 
> 
> Assuming the wf gives us correct probability results, it's surely the case 
> that it gives us information, what is the argument hat it also has physical 
> reality, whatever that means. What does physical reality mean here, without 
> resorting to your arithmetic theory? AG


If you make a series of up/down measurement of particles in the state up + 
down, the result is the same as for a mixture of particles in the up and down 
state. A mixture of particles in the up and down state would give the same 
result. Yet, if we decide to measure in the complementary base up’ /down’, we 
get quite different result. The superposition up + down = up’, so with the 
up’/down’, all particles up + down will go through, when only half of them go 
through with the mixture. So the difference between mixture and superposition 
has to be considered as a physical reality. Physical reality is simply what we 
observe.










>>> 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.
> 
> 
> The interferences are between waves, not state.
> 
> 
> We're doing Wave Mechanics, where the state functions are also called WAVE 
> functions, so the interference, if it exists, is between states or wf’s.

Fair enough.


> In the case of vectors in the plane, orthogonality between two vectors means 
> 90 degrees in separation. These vectors don't interfere because they are 
> orthogonal -- defined as the dot product, aka, inner product, which is zero. 
> So, in a quantum superposition, whether there is interference between the 
> components depends on whether there is mutual interference as defined by the 
> inner product. In standard QM, the superposition is understood, or usually 
> written, as sums of orthogonal states. So no interference. Correct me if I am 
> wrong, or if you disagree. AG

I sort of agree, but the language is non standard. We prefer to say that 
orthogonal state interfere through their possible superposition. It is the 
orthogonal states which are said to interfere through their possible 
superposition. In the two slits experience, we make the particle in slit one 
position interfere with particle in slit two position, because the wave of that 
(one) particles describes a superposition of the two positions/path. 




> 
> 
> With the spin Up can be written as superpositions, like
> 
> Up = 1/sqrt(2) Up’ + 1/sqrt(2) Down
> Down =  1/sqrt(2) Up’ - 1/sqrt(2) Down
> 
> What is Up'? So the wf for spin, which is Up + Dn (leaving out normalization 
> factor) is, you now imply, 2/sqrt(2) Up'. Make no sense. CMIIAW. AG 

Up’ = up - down
Down’ = up +down

It is the usual “complementarily”, like a precise position is a superposition 
of all momenta, and a precise momentum is a superposition of all position. It 
is a change of base. (Leaving out the normalisation factor).

It is the base after some pi/4 rotation, for example.




> 
> The interference comes from sum and difference of such superpositions. 
> 
> Take the two “orthogonal” slits: in classical physics you can add up and 
> multiply he probabilities in the usual way for the alternatives and sequence 
> of events, but in quantum mechanics, you have an amplitude, which describes a 
> “wave of history”, and to predict the final state, you need to square the 
> amplitude, and this takes into account all path, basically because (a+ b)^2 
> is different from a^2 + b^2.
> 
> 
> 
>> 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 
> 
> I don’t really understand the language. You have interference when the wave 
> of a particle describe different outcomes possible for some observable.
> 
> I think this is wrong. See my above comment about orthogonality. Writing a 
> superposition as a sum of possible eigenstates does not necessarily imply 
> interference, not if the states are orthogonal, which is usually assumed. AG


The point is that up cannot be orthogonal with up + down, nor with up - down.



>  
> If it is the position, like in the two slits, interference comes from the 
> existence of state “superposing” two (or more) states from the base. The 
> interference is, somehow, the superposition itself, when recombined at some 
> place (screen, interferometer, etc.)
> 
> In the double slit, there IS interference between the waves exiting from each 
> slit. But IMO this should not be generalized for all superpositions of 
> quantum systems.


Well, it is, except for special selection rules, charges, etc. 



> As I wrote, I believe that from this seminal experiment, arose the general 
> interpretation of superposition, which I contest. So far, I have not seen any 
> justification of this extension.


See above. We need to distinguish mixture and superposition. They gave 
different predictions.


> It leads to the false belief IMO, that systems in superpositions are 
> simultaneously in all component states, from which we the MWI and cats alive 
> and dead simultaneously. 

Indeed. 



> In the latter case, Brent claimed that Schroedinger got it wrong, and that 
> decoherence theory explains it by asserting the cat is in the apparently 
> contradictory state for only fractions of nano seconds,

If the cat alive/dead is correlated with some up+down state, the cat state 
becomes alive +dead, FOREVER. When a superposition appears, it never 
disappears. 




> so we never see that state.

Brent is right on this. We never see that state because our bodies/brain use 
the position base, and we get ourself superposed, and QM explains why we don’t 
feel that way, like Mechanism explains we cannot feel to be both in W and M 
after duplication. The non)collapse theory interprets superposition by 
“ignorance” of which branch we are in.




> IMO, this explanation doesn't work for several reasons, one of which is that 
> the wf used in decoherence theory assumes the measuring device is put in 
> place before decoherence occurs. But how is this possible with such a short 
> decoherence time?

Decoherence is not collapse. You just need to isolate yourself (and the 
measurement device) from the particles. It is obviously non feasible for hot 
macroscopic object, which implies a quick decoherence time, but the 
superposition do not disappear, they only get useless from the point of view of 
an observer. In principle, by erasing his memory of the cat state, measuring in 
the dead+alive, dead-alive base, we could resurrect the cat. That has been 
done, but only with microscopic cats.



> Long before the device is attached and the experiment is performed, it has 
> interacted with the environment, meaning that the wf on which decoherence is 
> based, is impossible to establish. AG  

? It is the universal wave. We just assume QM applies on everything here. Then 
we can uderstad why macro-superposition are not observable, for obvious 
statistical/thermodynamical reasons.

Bruno



> 
> Do you know the book by David Albert “Quantum Mechanics and Experience”, it 
> is quite good pedagogically, and he explains well the “problem”. He dmisloh 
> Everett very badly (good for Everett!), and defend Bohm quite unconvincingly 
> (for me at least). But he introduces very well the basic core theory, using 
> only very elementary algebra.
> 
> Bruno
> 
> 
> 
>> 
> 
> 
> 
> 
> 
> 
> 
> 
>> 
>> 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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