On Wednesday, November 28, 2018 at 1:46:28 PM UTC, Bruno Marchal wrote:
>
>
> On 26 Nov 2018, at 22:49, [email protected] <javascript:> wrote:
>
>
>
> On Monday, November 26, 2018 at 9:43:14 PM UTC, [email protected] wrote:
>>
>>
>>
>> On Monday, November 26, 2018 at 4:41:42 PM UTC, [email protected] 
>> wrote:
>>>
>>>
>>>
>>> On Monday, November 26, 2018 at 12:01:05 PM UTC, Bruno Marchal wrote:
>>>>
>>>>
>>>> On 23 Nov 2018, at 13:30, [email protected] wrote:
>>>>
>>>>
>>>>
>>>> On Friday, November 23, 2018 at 11:29:14 AM UTC, Bruno Marchal wrote:
>>>>>
>>>>>
>>>>> On 21 Nov 2018, at 18:03, [email protected] wrote:
>>>>>
>>>>>
>>>>>
>>>>> On Monday, November 19, 2018 at 3:52:37 PM UTC, Bruno Marchal wrote:
>>>>>>
>>>>>>
>>>>>> On 18 Nov 2018, at 14:00, [email protected] wrote:
>>>>>>
>>>>>>
>>>>>>
>>>>>> On Sunday, November 18, 2018 at 12:19:20 PM UTC, Bruno Marchal wrote:
>>>>>>>
>>>>>>>
>>>>>>> On 16 Nov 2018, at 15:38, [email protected] wrote:
>>>>>>>
>>>>>>>
>>>>>>>
>>>>>>> On Friday, November 16, 2018 at 10:14:32 AM UTC, scerir wrote:
>>>>>>>>
>>>>>>>>
>>>>>>>> Il 16 novembre 2018 alle 10.19 [email protected] ha scritto: 
>>>>>>>>
>>>>>>>>
>>>>>>>>
>>>>>>>> On Thursday, November 15, 2018 at 2:14:48 PM UTC, scerir wrote:
>>>>>>>>
>>>>>>>>
>>>>>>>> Il 15 novembre 2018 alle 14.29 [email protected] ha scritto: 
>>>>>>>>
>>>>>>>>
>>>>>>>>
>>>>>>>> On Thursday, November 15, 2018 at 8:04:53 AM UTC, scerir wrote:
>>>>>>>>
>>>>>>>> Imagine a spin-1/2 particle described by the state psi = sqrt(1/2) 
>>>>>>>> [(s+)_z + (s-)_z] .
>>>>>>>>
>>>>>>>> If the x-component of spin is measured by passing the spin-1/2 
>>>>>>>> particle through a Stern-Gerlach with its field oriented along the 
>>>>>>>> x-axis, 
>>>>>>>> the particle will ALWAYS emerge 'up'.
>>>>>>>>
>>>>>>>>
>>>>>>>> *Why?  Won't the measured value be along the x axis in both 
>>>>>>>> directions, in effect Up or Dn? AG*
>>>>>>>>
>>>>>>>> "Hence we must conclude that the system described by the |+>x state 
>>>>>>>> is not the
>>>>>>>> same as a mixture of atoms in the |+> and !-> states. This means 
>>>>>>>> that each atom in the
>>>>>>>> beam is in a state that itself is a combination of the |+> and |-> 
>>>>>>>> states. A superposition
>>>>>>>> state is often called a coherent superposition since the relative 
>>>>>>>> phase of the two terms is
>>>>>>>> important."
>>>>>>>>
>>>>>>>> .see pages 18-19 here *https://tinyurl.com/ybm56whu 
>>>>>>>> <https://tinyurl.com/ybm56whu>*
>>>>>>>>
>>>>>>>>
>>>>>>>> *Try answering in your own words. When the SG device is oriented 
>>>>>>>> along the x axis, now effectively the z-axix IIUC, and we're dealing 
>>>>>>>> with 
>>>>>>>> superpositions, the outcomes will be 50-50 plus and minus. Therefore, 
>>>>>>>> unless I am making some error, what you stated above is incorrect. AG *
>>>>>>>>
>>>>>>>> sqrt(1/2) [(s+)_z +(s-)_z]  is a superposition, but since sqrt(1/2) 
>>>>>>>> [(s+)_z +(s-)_z]  =  (s+)_x the particle will always emerge 'up'
>>>>>>>>
>>>>>>>
>>>>>>> I'll probably get back to on the foregoing. In the meantime, 
>>>>>>> consider this; I claim one can never MEASURE Up + Dn or Up - Dn with a 
>>>>>>> SG 
>>>>>>> apparatus regardless of how many other instruments one uses to create a 
>>>>>>> composite measuring apparatus (Bruno's claim IIUC). The reason is 
>>>>>>> simple. 
>>>>>>> We know that the spin operator 
>>>>>>>
>>>>>>>
>>>>>>> Which one? 
>>>>>>>
>>>>>>
>>>>>> *Good question. AG*
>>>>>>
>>>>>> There are spin operator for each direction in space. The 
>>>>>>> superposition of up and down is a precise pure state, with precise 
>>>>>>> eigenvalues, when measuring state in the complementary directions.
>>>>>>>
>>>>>>
>>>>>> *As I wrote earlier, based on scerir's superpositions on different 
>>>>>> axes, and simulation, I now think that Up + Dn and Up - Dn can be 
>>>>>> measured 
>>>>>> along the x axis but not along the z axis (which I was focused on). *
>>>>>>
>>>>>>
>>>>>> All you need to do is a change of base. The operator will be defined 
>>>>>> clearly by the Eigen value on the diagonal in the corresponding base. 
>>>>>> You 
>>>>>> can prepare any state, and measure them “in any base”. 
>>>>>>
>>>>>
>>>>>
>>>>> *I'll get back to this issue in my next post. AG *
>>>>>
>>>>>> *You were probably correct about x axis measurements, but perhaps 
>>>>>> were not clear enough. You were not explicit that measurements along the 
>>>>>> x 
>>>>>> axis is a different SG experiment from along z axis.*
>>>>>>
>>>>>>
>>>>>> OK. Sorry. 
>>>>>>
>>>>>> * I thought you meant do them in succession, not as separate 
>>>>>> experiments.*
>>>>>>
>>>>>>
>>>>>> Ah? OK.
>>>>>>
>>>>>>
>>>>>> * Also introducing an infinity of universes seems extraneous and 
>>>>>> confusing for a solution to this problem. AG *
>>>>>>
>>>>>> I are probably different on this. I don’t take the word “universe” 
>>>>>> too much seriously, as with mechanism we know at the start that there is 
>>>>>> “physical universe” at all, just the natural numbers with the laws of 
>>>>>> addition and multiplication. Both the computational and the quantum 
>>>>>> state 
>>>>>> are relative, and high level, pertaining to what is “observable” for 
>>>>>> some 
>>>>>> the point of view of some locally finite subject, run by some 
>>>>>> computation.
>>>>>>
>>>>>> The empirical point, though, is that to predict correctly an event in 
>>>>>> quantum mechanics, we have to take into account may simultaneous 
>>>>>> “incompatible path”, like going through each hole in a plane. Quantum 
>>>>>> computations, for example, exploits that seemingly parallelism. 
>>>>>>
>>>>>
>>>>> *I don't like this approach -- in fact I abhor it -- since it implies 
>>>>> simultaneous interference among a multitude of paths to the same point on 
>>>>> the detection screen. This adds an unnecessary mystery to QM. In the 
>>>>> Hilbert Space representation, the wf is what it is, but can be 
>>>>> represented 
>>>>> in a multitude of different bases. It is therefore misleading to claim 
>>>>> the 
>>>>> system being analyzed is in a multitude of states; rather it is in one 
>>>>> state, which due to linear algebra, has many representations. AG *
>>>>>
>>>>>
>>>>>
>>>>> I can be OK with this, if you agree that the consciousness of the 
>>>>> observer is relatively associated to those representations, in the base 
>>>>> “chosen” by nature in the evolution of the brain. That gives rise to the 
>>>>> “relative state” view of QM.
>>>>>
>>>>
>>>> *I don't agree. I am not even sure what you mean. You don't need a 
>>>> conscious observer to detect the results of a slit experiment. *
>>>>
>>>>
>>>> Did I say that?
>>>>
>>>
>>> *IMO yes. You asserted the need for an observer. The interference 
>>> pattern exists if there are no observers. It's like saying the Moon exists 
>>> even if no one ever looks at it, which was the situation throughout most of 
>>> the Moon's lifetime. AG *
>>>
>>>>
>>>>
>>>>
>>>> *All you need is a detector to record the results. Feynman made this 
>>>> point and I don't see anything problem with this logic.*
>>>>
>>>> I agree with Feynman and Everett on this. It is the advantage of NOT 
>>>> believing in the wave reduction: consciousness is entirely handle by the 
>>>> Mechanist theory of mind. But then we can associate consciousness to the 
>>>> apprehension of the distinction brought by the measuring apparatus, in all 
>>>> branches of the superposition, and you get the “many-worlds” or the 
>>>> “many-relative-histories”.
>>>>
>>>
>>> *Where in Feynman's postulates does he assert or infer no wave packet 
>>> reduction? I have to check his postulates, but if he really developed a 
>>> particle-only theory, there are no wave packets. AG *
>>>
>>>> *The problem IMO with sums over histories is that it adds a superfluous 
>>>> mystery (in spades) to the results, say, of a slit experiment. We still 
>>>> have the mystery as to why interference for every point along the screen 
>>>> in 
>>>> a single trial, yields a single impact. But with sums over histories IIUC, 
>>>> for each impact point or result, we also have an infinite set of histories 
>>>> which the particle is in simultaneously. I don't see that anything has 
>>>> been 
>>>> gained, other than having an additional baffling mystery used to sell 
>>>> books 
>>>> which confuse the lay public as well as professional physicists. AG*
>>>>
>>>>
>>>> It is just QM without reduction of the wave packet. If there is no wave 
>>>> packet reduction, you get the relative states, including consciousness 
>>>> differentiation, using just the mechanist theory of mind (the oldest 
>>>> theory 
>>>> of mind).
>>>>
>>>
>>> *You're reading much too much into Sums Over Histories (or Relative 
>>> Dtates) to reach this conclusion. CMIIAW, but Feynman discovered another 
>>> way to calculate probabilities. He didn't, and couldn't explain why we get 
>>> one result and not another in, say, a slit experiment. At best he was 
>>> neutral as to what happens to the wf at measurement time, since, IIUC, he 
>>> has no wf's in his theory. AG*
>>>
>>
>> *I checked the postulates in Feynman's Sums Over Histories (in link 
>> provided by Phil) and I see nothing related to waves, as expected, and thus 
>> nothing about collapse of anything. I would suppose the same applies to 
>> Heisenberg's Matrix Mechanics; no waves, no collapse. I suppose you could 
>> say they just produce correct probabilities, and imply nothing about 
>> relative states other than their probabilities (which wave mechanics does), 
>> but certainly nothing about consciousness. To summarize: you're right that 
>> they are "no collapse" theories, but IMO they say nothing about 
>> consciousness. AG*
>>
>
> *One final point; In wave mechanics, I think you find the "disappearance" 
> of the Schrodinger equation at moment of collapse troubling. But if you 
> have varying probabilities, say for a horse race (Bruce's example), when 
> the winner crosses the finish line, the probabilities cease to vary. Isn't 
> this sort of what's expected of the Schrodinger equation at measurement 
> time? AG* 
>
>
>
> If there is no collapse, the disappearance is explained 
> phenomenologically, but there is no ontological disappearance, and that it 
> is good, because we know that all terms of the waves are needed to get the 
> predictions exact.
>
> It is very simple: any collapse postulate is equivalent with saying that 
> the QM (schroedinger/heisnberg/feynman formalism)  is wrong. 
>


*If you don't like collapse, then don't use Wave Mechanics, but 
Heisenberg's or Feynman's formulation of QM. I think you're creating a 
problem for yourself. AG*

The collapse can only violate the linearity of the evolution and tensor 
> products. That’s why Boher insisted that QM does not apply to macroscopic 
> observers, but as Einstein shows, that makes not much sense, unless 
> accepting spooky action at a distance, a god who plays with dice and/or 
> that physics talk about mind, and never nature.
>
> Bruno
>
>
>
>
>
>
>>
>>>  
>>>
>>>>
>>>>
>>>>
>>>>
>>>>
>>>>
>>>>
>>>>
>>>> has exactly two eigenstates, each with probability of .5. We can write 
>>>>>>> them down. We also know that every quantum measurement gives up an 
>>>>>>> eigenvalue of some eigenstate. Therefore, if there existed an Up + Dn 
>>>>>>> or Up 
>>>>>>> - Dn eigenstate, it would have to have probability ZERO since the Up 
>>>>>>> and Dn 
>>>>>>> eigenstates have probabilities which sum to unity. Do you agree or not, 
>>>>>>> and 
>>>>>>> if not, why? TIA, AG 
>>>>>>>
>>>>>>>
>>>>>>> You add the probabilities, but you need to add the amplitudes of 
>>>>>>> probabilities instead, and then take their square. You simply dismiss 
>>>>>>> the 
>>>>>>> quantum formalism, it seems to me. 
>>>>>>>
>>>>>>
>>>>>> *I did not; an incorrect inference on your part.*
>>>>>>
>>>>>> All right. (I was just trying to figure out what you did, to be sure).
>>>>>>
>>>>>> *I** never mentioned Born's rule (it wasn't necessary), *
>>>>>>
>>>>>>
>>>>>> You did use the probability 1/2 at some place, with the particle in a 
>>>>>> state 1/sqrt(2)(up + down). We use all the time the Born rule when we 
>>>>>> talk 
>>>>>> about measurement. 
>>>>>>
>>>>>
>>>>>
>>>>> *I just assumed a probability of .5 for Up and Dn states after 
>>>>> application of Born's rule. AG *
>>>>>
>>>>>
>>>>> That was my point.
>>>>>
>>>>
>>>> *Your point, IIUC, was that I was denying the postulates of QM by 
>>>> ignoring Born's Rule, but I was not doing that. I just chose not to 
>>>> mention 
>>>> it. Nothing more. AG *
>>>>
>>>>
>>>> OK, then.
>>>>
>>>> Bruno
>>>>
>>>>
>>>>
>>>>
>>>>> Bruno
>>>>>
>>>>> PS I got a mail back as undelivered. I will try to resend it later.
>>>>>
>>>>>
>>>>>
>>>>>
>>>>>
>>>>>> *from which one cannot infer I am criticizing QM itself. AG *
>>>>>>
>>>>>>
>>>>>> I am just trying to understand what you don’t understand, which is 
>>>>>> not easy in a context where the more we understand the formalism, the 
>>>>>> less 
>>>>>> we understand what it could mean, even more so if we give sense to a 
>>>>>> dualist wave packet reduction. 
>>>>>>
>>>>>> I am a logician: it is clear that Copenhagen and Everett are not two 
>>>>>> different interpretations, but two different theories. One is 
>>>>>> Schroedinger 
>>>>>> equation + wave packet reduction + a dualist theory of 
>>>>>> mind/observation), 
>>>>>> the other is just Schroedinger equation only + the “usual” mechanist 
>>>>>> theory 
>>>>>> of mind. There are many possible debate on all his of course.
>>>>>>
>>>>>> I urge you to study the treatment of the interferometer in David 
>>>>>> Albert books. It is weird. Bohr is right on this: to understand it means 
>>>>>> to 
>>>>>> get the point that is hard to figure out how nature could to that, but 
>>>>>> from 
>>>>>> the mechanist post Gödel view, it is rather natural, as we observe is 
>>>>>> given 
>>>>>> by a statistics on infinitely many computations/histories. 
>>>>>>
>>>>>> Bruno
>>>>>>
>>>>>>
>>>>>>
>>>>>>
>>>>>>
>>>>>> The states constituted a vector space: the sum (superposition) of 
>>>>>>> orthogonal states are pure state, after a change of base, and I did 
>>>>>>> give 
>>>>>>> you the corresponding operator. You are not criticising an 
>>>>>>> interpretation 
>>>>>>> of QM, but QM itself.
>>>>>>>
>>>>>>
>>>>>>
>>>>>>> Bruno
>>>>>>>
>>>>>>>
>>>>>>>
>>>>>>>
>>>>>>>
>>>>>>>>
>>>>>>>>   
>>>>>>>>
>>>>>>>> In fact (s+)_z = sqrt(1/2) [(s+)_x + (s-)_x]
>>>>>>>>
>>>>>>>> and (s-)_z = sqrt(1/2) [(s+)_x - (s-)_x]
>>>>>>>>
>>>>>>>> (where _z, _x, are the z-component and the x-component of spin)
>>>>>>>>
>>>>>>>> so that psi = sqrt(1/2)[(s+)_z +(s-)_z] = (s+)_x.   (pure state, 
>>>>>>>> not mixture state)..
>>>>>>>>
>>>>>>>> AGrayson2000 asked "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?"
>>>>>>>>
>>>>>>>> Does Everett's "relative state interpretation" show how to 
>>>>>>>> interpret a real superposition (like the above, in which the particle 
>>>>>>>> will 
>>>>>>>> always emerge 'up') and how to interpret a mixture (in which the 
>>>>>>>> particle 
>>>>>>>> will emerge 50% 'up' or 50% 'down')?
>>>>>>>>
>>>>>>>>  
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