On Thursday, December 6, 2018 at 5:46:13 PM UTC, [email protected] wrote:
>
>
>
> On Wednesday, December 5, 2018 at 10:13:57 PM UTC, [email protected] 
> wrote:
>>
>>
>>
>> On Wednesday, December 5, 2018 at 9:42:51 PM UTC, Bruce wrote:
>>>
>>> On Wed, Dec 5, 2018 at 10:52 PM <[email protected]> wrote:
>>>
>>>> On Wednesday, December 5, 2018 at 11:42:06 AM UTC, [email protected] 
>>>> wrote:
>>>>>
>>>>> On Tuesday, December 4, 2018 at 9:57:41 PM UTC, Bruce wrote:
>>>>>>
>>>>>> On Wed, Dec 5, 2018 at 2:36 AM <[email protected]> wrote:
>>>>>>
>>>>>>>
>>>>>>> *Thanks, but I'm looking for a solution within the context of 
>>>>>>> interference and coherence, without introducing your theory of 
>>>>>>> consciousness. Mainstream thinking today is that decoherence does 
>>>>>>> occur, 
>>>>>>> but this seems to imply preexisting coherence, and therefore 
>>>>>>> interference 
>>>>>>> among the component states of a superposition. If the superposition is 
>>>>>>> expressed using eigenfunctions, which are mutually orthogonal -- 
>>>>>>> implying 
>>>>>>> no mutual interference -- how is decoherence possible, insofar as 
>>>>>>> coherence, IIUC, doesn't exist using this basis? AG*
>>>>>>>
>>>>>>
>>>>>> I think you misunderstand the meaning of "coherence" when it is used 
>>>>>> off an expansion in terms of a set of mutually orthogonal eigenvectors. 
>>>>>> The 
>>>>>> expansion in some eigenvector basis is written as
>>>>>>
>>>>>>    |psi> = Sum_i (a_i |v_i>)
>>>>>>
>>>>>> where |v_i> are the eigenvectors, and i ranges over the dimension of 
>>>>>> the Hilbert space. The expansion coefficients are the complex numbers 
>>>>>> a_i. 
>>>>>> Since these are complex coefficients, they contain inherent phases. It 
>>>>>> is 
>>>>>> the preservation of these phases of the expansion coefficients that is 
>>>>>> meant by "maintaining coherence". So it is the coherence of the 
>>>>>> particular 
>>>>>> expansion that is implied, and this has noting to do with the mutual 
>>>>>> orthogonality or otherwise of the basis vectors themselves. In 
>>>>>> decoherence, 
>>>>>> the phase relationships between the terms in the original expansion are 
>>>>>> lost.
>>>>>>
>>>>>> Bruce 
>>>>>>
>>>>>
>>>>> I appreciate your reply. I was sure you could ascertain my error -- 
>>>>> confusing orthogonality with interference and coherence. Let me have your 
>>>>> indulgence on a related issue. AG
>>>>>
>>>>
>>>> Suppose the original wf is expressed in terms of p, and its 
>>>> superposition expansion is also expressed in eigenfunctions with variable 
>>>> p. Does the phase of the original wf carry over into the eigenfunctions as 
>>>> identical for each, or can each component in the superposition have 
>>>> different phases? I ask this because the probability determined by any 
>>>> complex amplitude is independent of its phase. TIA, AG 
>>>>
>>>
>>> The phases of the coefficients are independent of each other.
>>>
>>
>> When I formally studied QM, no mention was made of calculating the phases 
>> since, presumably, they don't effect probability calculations. Do you have 
>> a link which explains how they're calculated? TIA, AG 
>>
>
> I found some links on physics.stackexchange.com which show that relative 
> phases can effect probabilities, but none so far about how to calculate any 
> phase angle. AG 
>

Here's the answer if anyone's interested. But what's the question? How are 
wf phase angles calculated? Clearly, if you solve for the eigenfunctions of 
some QM operator such as the p operator, any phase angle is possible; its 
value is completely arbitrary and doesn't effect a probability calculation. 
In fact, IIUC, there is not sufficient information to solve for a unique 
phase. So, I conclude,that the additional information required to uniquely 
determine a phase angle for a wf, lies in boundary conditions. If the 
problem of specifying a wf is defined as a boundary value problem, then, I 
believe, a unique phase angle can be calculated. CMIIAW. AG 

>
>>> Bruce
>>>
>>>  
>>>
>>

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