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* 

>
>
>>  
>>
>>>
>>>
>>>
>>>
>>>
>>>
>>>
>>>
>>> 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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