On Tuesday, December 5, 2017 at 5:32:22 AM UTC, [email protected] wrote:
>
>
>
> On Tuesday, December 5, 2017 at 3:59:19 AM UTC, [email protected] wrote:
>>
>>
>>
>> On Tuesday, December 5, 2017 at 12:50:54 AM UTC, Bruce wrote:
>>>
>>> On 5/12/2017 11:38 am, [email protected] wrote:
>>>
>>> On Tuesday, December 5, 2017 at 12:26:58 AM UTC, Bruce wrote: 
>>>>
>>>> On 5/12/2017 3:15 am, Bruno Marchal wrote: 
>>>> > On 01 Dec 2017, at 01:49, Bruce Kellett wrote: 
>>>> >> On 1/12/2017 8:57 am, Bruce Kellett wrote: 
>>>> >>> On 1/12/2017 4:21 am, Bruno Marchal wrote: 
>>>> >>>> On 29 Nov 2017, at 23:16, Bruce Kellett wrote: 
>>>> >>>> On 30/11/2017 2:24 am, Bruno Marchal wrote: 
>>>> >>>>>> On 29 Nov 2017, at 04:59, Bruce Kellett wrote: 
>>>> >>>>>> 
>>>> >>>>>>> I would suggest that there is no such world. Whether a coin 
>>>> >>>>>>> comes up head or tails on a simple toss is not a quantum event; 
>>>> >>>>>>> it is determined by quite classical laws of physics governing 
>>>> >>>>>>> initial conditions, air currents and the like. 
>>>> >>>>>> 
>>>> >>>>>> It depends. If you shake the coin long enough, the quantum 
>>>> >>>>>> uncertainties can add up to the point that the toss is a quantum 
>>>> >>>>>> event. With some student we have evaluate this quantitavely (a 
>>>> >>>>>> long time ago) and get that if was enough to shake the coin less 
>>>> >>>>>> than a minute, but more than few seconds ... (Nothing rigorous). 
>>>> >>>>> 
>>>> >>>>> That is a misunderstanding of quantum randomness. For the outcome 
>>>> >>>>> of a coin toss to be determined by quantum randomness, we would 
>>>> >>>>> have to have a single quantum event where the outcome was 
>>>> >>>>> amplified by decoherence so that it was directly entangled with 
>>>> >>>>> the way the coin landed. Schematically: 
>>>> >>>>> 
>>>> >>>>>  |quantum event>|coin> = (|outcome A> + |outcome B>)|coin> 
>>>> >>>>>  = (|outcome A>|coin heads> + |outcome B>|coin tails>) 
>>>> >>>> 
>>>> >>>> The coin is quantum. 
>>>> >>> 
>>>> >>> The coin is classical, consisting of something of the order of 
>>>> 10^22 
>>>> >>> atoms. Indeterminacy in position as given by the Heisenberg 
>>>> >>> Uncertainty Principle, is undetectably small. 
>>>> >> 
>>>> >> I think it is worth while to put some (approximate) numbers around 
>>>> >> this. The reduced Planck constant, h-bar, is approximately 10^{-27} 
>>>> >> g.cm^2/s. The Uncertainty Principle is 
>>>> >> 
>>>> >>    delta(x)*delta(p) >= h-bar/2. 
>>>> >> 
>>>> >> For a coin weighing approximately 10 g and moving at 1 cm/s, the 
>>>> >> momentum is mv = 10 g.cm/s. Taking the momentum uncertainty to be 
>>>> of 
>>>> >> this order, the uncertainty in position, delta(x) is of the order of 
>>>> >> 10^{-28} cm. A typical atom has a diameter of about 10^{-8} cm, so 
>>>> >> the uncertainty in position is approximately 20 orders of magnitude 
>>>> >> less than the atomic diameter. 
>>>> > 
>>>> > I think that is enough to get the macroscopic superposition, as, like 
>>>> > I explained, you have to take into account not just the quantum 
>>>> > indeterminacy, + the classical chaos. You might need to shake for 
>>>> some 
>>>> > minutes. 
>>>>
>>>> You could shake for longer than the age of the universe and you will 
>>>> still not convert quantum uncertainties and classical thermal motions 
>>>> into a macroscopic superposition. Do you know nothing about coherence? 
>>>> And the fact that coherent phases between the components are what 
>>>> separates a superposition from a mixture?
>>>
>>>
>>> Are the phase angles of components of a superposition identical? If so, 
>>> is this the definition of coherence? TIA, AG
>>>
>>>
>>> No, why should they be equal. You really do have to learn some basic 
>>> quantum mechanics, Alan, and stop bothering the list with such questions.
>>>
>>> Bruce
>>>
>>
>> Was I bothering the list when I started this thread, and others? I recall 
>> from class the answer is NO, because the probabilities are unaffected when 
>> taking complex conjugates (ignoring interference), but other comments on 
>> Avoid2 for example, when I was a member, indicated otherwise. Also, the 
>> poster here you're replying to seemed not to understand as well. Next time 
>> take THAT into account. AG 
>>
>
> I took a few graduate courses in QM at major US universities and do not 
> recall any discussion about coherent states of superposition when solving 
> the SWE or Dirac's equation. Maybe the universities in Australia do a 
> better job. I suggest you be more tolerant in the future, notwithstanding 
> the burden that your knowledge of these subjects places on your karma. And 
> keep in mind that I am responsible the interactions you are now enjoying. 
> That should count for something. Don't ya think? FWIW, I initially left 
> Avoid2 because of the abuse. AG 
>

All I can recall about the phase factor in QM is that it's arbitrary, 
insofar as whatever value is chosen doesn't effect the result of Born's 
rule. I suppose that makes me a moron from the pov of an expert. The 
implication was, for me, that it can't be explicitly calculated. Hence, my 
question. AG


>>> Random quantum uncertainties 
>>>> and thermal motions are not coherent, so cannot form superpositions. 
>>>>
>>>

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