On Saturday, November 25, 2017 at 7:11:52 PM UTC, Lawrence Crowell wrote:
>
> On Saturday, November 25, 2017 at 11:55:47 AM UTC-6, agrays...@gmail.com 
> wrote:
>>
>>
>>
>> On Saturday, November 25, 2017 at 3:06:50 PM UTC, Lawrence Crowell wrote:
>>>
>>> On Thursday, November 23, 2017 at 9:21:14 PM UTC-6, agrays...@gmail.com 
>>> wrote:
>>>>
>>>>
>>>>
>>>> On Thursday, November 23, 2017 at 11:15:40 PM UTC, Lawrence Crowell 
>>>> wrote:
>>>>>
>>>>>
>>>>>
>>>>> I am new to this list and have not followed all the arguments here. In 
>>>>> weighing in here I might be making an error of not addressing things 
>>>>> properly. 
>>>>>
>>>>> Consider quantum entanglements, say the entanglements of two spin 1/2 
>>>>> particles. In the singlet state |+>|-> + |->|+> we really do not have the 
>>>>> two spin particles. The entanglement state is all that is identifiable. 
>>>>> The 
>>>>> degrees of freedom for the two spins are replaced with those of the 
>>>>> entanglement state. It really makes no sense to talk about the individual 
>>>>> spin particles existing. If the observer makes a measurement that results 
>>>>> in a measurement the entanglement state is "violently" lost, the 
>>>>> entanglement phase is transmitted to the needle states of the apparatus, 
>>>>> and the individual spin degrees of freedom replace the entanglement. 
>>>>>
>>>>> We have some trouble understanding this, for the decoherence of the 
>>>>> entangled state occurs with that state as a "unit;" it is blind to any 
>>>>> idea 
>>>>> there is some "geography" associated with the individual spins. There in 
>>>>> fact really is no such thing as the individual spins. The loss of the 
>>>>> entangled state replaces that with the two spin states. Since there is no 
>>>>> "metric" specifying where the spins are before the measurement there is 
>>>>> no 
>>>>> sense to ideas of any causal action that ties the two resulting spins. 
>>>>>
>>>>> This chaffs our idea of physical causality, but this is because we are 
>>>>> thinking in classical terms. There are two ways of thinking about our 
>>>>> problem with understanding whether quantum mechanics is ontic or 
>>>>> epistemic. 
>>>>>
>>>>
>>>> The fact that probability waves evolve and interfere with each other, 
>>>> and effect ensembles but not individual members, is inherently baffling. 
>>>> So 
>>>> the wf can't be completely epistemic since it modifies physical reality. 
>>>> That is, It must be ontic in some respect, but in ways that defy rational 
>>>> analysis. AG
>>>>
>>>
>>> I think you are falling into a trap that David Hume warns against. 
>>> Causality gives rise to correlation, but correlation is not necessarily the 
>>> result of causality. There is no effect or some causal principle at work 
>>> with either individual wave functions or wave functions in an ensemble of 
>>> experiments. The ensemble of experiments, the classic case being the two 
>>> slit experiment, is meant to deduces the wave nature of the quantum 
>>> physics. It is not there to deduce some causal influence underlying quantum 
>>> nonlocality. 
>>>
>>> LC
>>>
>>
>> Applying deBroglie's formula, a change in p changes the wave length, and 
>> thus the distribution on the screen. That is, the ensemble responds to 
>> changes in the wave length due to interference. I therefore deduce that the 
>> wave length has a physical effect on the ensemble, but not on individual 
>> outcomes. AG
>>
>
> You continue to make the error of thinking there must be some physical 
> effect in a measurement. 
>

 In a particular measurement outcome?  expressly denied that. I stated the 
physical effect of the wf is only discernible for ensembles. AG

The outcomes will obey a statistical distribution that is reflected in an 
> ensemble of experiments. The statistical distribution is predicted by the 
> nature of the wave function prior to a measurement. The wave function can 
> be interpreted in a ψ-epistemic sense (Copenhagen, Qubism etc) as only 
> telling you what information can be accessed from the quantum system. In a 
> ψ-ontic sense (MWI, Bohm etc) the wave function exists and evolves to 
> define possible outcomes, but the observer is not able to access any 
> predictive information as this necessitates some local hidden variable that 
> does not exist. What outcome happens in any particular measurements is not 
> predictable; there exists no causal principle which can tell you how a 
> particular outcome obtains. 
>

I never alleged otherwise. AG
 

> The occurrence of a statistical distribution of outcomes from an ensemble 
> of measurements does not mean there is some causal influence directing 
> outcomes. 
>

If the ensemble's distribution changes as a consequence of changes in the 
wf, IMO there is reason to believe the wf has ontic properties. That's all 
I was alleging. AG
 

> This distribution only obtains as a consequence of what the wave function 
> tells you (ψ-epistemology) about the system before measurement, or how the 
> wave function evolves as a physical system (ψ-ontology) prior to 
> measurement. It is my thinking that QM fails to completely live up to 
> either of these.
>
> LC
>

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