On Wednesday, December 5, 2018 at 12:53:45 AM UTC-6, Bruce wrote:
>
> On Wed, Dec 5, 2018 at 5:43 PM Philip Thrift <[email protected] 
> <javascript:>> wrote:
>
>> On Wednesday, December 5, 2018 at 12:28:19 AM UTC-6, Bruce wrote:
>>>
>>> On Wed, Dec 5, 2018 at 5:19 PM Philip Thrift <[email protected]> wrote:
>>>
>>>> On Wednesday, December 5, 2018 at 12:00:18 AM UTC-6, Bruce wrote:
>>>>>
>>>>> On Wed, Dec 5, 2018 at 4:51 PM Philip Thrift <[email protected]> 
>>>>> wrote:
>>>>>
>>>>>> On Tuesday, December 4, 2018 at 11:39:43 PM UTC-6, Bruce wrote:
>>>>>>>
>>>>>>> On Wed, Dec 5, 2018 at 3:53 PM Philip Thrift <[email protected]> 
>>>>>>> wrote:
>>>>>>>
>>>>>>>> On Tuesday, December 4, 2018 at 10:28:39 PM UTC-6, Philip Thrift 
>>>>>>>> wrote:
>>>>>>>>>
>>>>>>>>> On Tuesday, December 4, 2018 at 3:45:32 PM UTC-6, Bruce wrote:
>>>>>>>>>>
>>>>>>>>>> On Wed, Dec 5, 2018 at 6:58 AM Philip Thrift <[email protected]> 
>>>>>>>>>> wrote:
>>>>>>>>>>
>>>>>>>>>>>
>>>>>>>>>>> On Tuesday, December 4, 2018 at 1:53:15 PM UTC-6, Brent wrote:
>>>>>>>>>>>>
>>>>>>>>>>>>
>>>>>>>>>>>> On 12/4/2018 12:25 AM, Philip Thrift wrote:
>>>>>>>>>>>>
>>>>>>>>>>>>
>>>>>>>>>>>> 1. Histories originate at an emitter e and end at screen 
>>>>>>>>>>>> locations s on a screen S.
>>>>>>>>>>>> 2. At each s there is a history bundle histories(s). A weight 
>>>>>>>>>>>> w(s) is computed from the bundle by summing the unit complex 
>>>>>>>>>>>> numbers of the 
>>>>>>>>>>>> histories and taking the modulus. 
>>>>>>>>>>>> 3. The weight w(s) is sent back in time over a single history 
>>>>>>>>>>>> h*(s) selected at random (uniformly) from histories(s).
>>>>>>>>>>>> 4. At e, the weights w(s) on backchannel of h*(s) are received 
>>>>>>>>>>>> (in the "present" time)
>>>>>>>>>>>> 5. A single history h*(s*) is then selected from the 
>>>>>>>>>>>> distribution in 4.
>>>>>>>>>>>>
>>>>>>>>>>>>
>>>>>>>>>>>> How is it selected?  Above you said "at random".  But that 
>>>>>>>>>>>> implies there is already a probability measure defined on the 
>>>>>>>>>>>> histories.  
>>>>>>>>>>>> How is this probability measure determined?  Or put another way 
>>>>>>>>>>>> how do you 
>>>>>>>>>>>> determine what histories to consider to form the bundles in step 2?
>>>>>>>>>>>>
>>>>>>>>>>>> Brent
>>>>>>>>>>>>
>>>>>>>>>>>
>>>>>>>>>>> Selection happens via quantum Darwinism. 
>>>>>>>>>>>
>>>>>>>>>>
>>>>>>>>>>
>>>>>>>>>> Do you have even the faintest understanding of Quantum Darwinism?
>>>>>>>>>>
>>>>>>>>>> Bruce 
>>>>>>>>>>
>>>>>>>>>
>>>>>>>>> How is *sum over histories with Darwinian selection*  (as 
>>>>>>>>> defined) not quantum Darwinism?
>>>>>>>>>
>>>>>>>>> Operationally, what is different?
>>>>>>>>>
>>>>>>>>> - pt
>>>>>>>>>
>>>>>>>>
>>>>>>>> *Sum over histories with Darwinian selection* is consistent with 
>>>>>>>> *Quantum 
>>>>>>>> Darwinism as a Darwinian process*  [ 
>>>>>>>> https://arxiv.org/abs/1001.0745 ].
>>>>>>>>
>>>>>>>
>>>>>>> No, you clearly don't understand Quantum Darwinism! Zurek's 
>>>>>>> Darwinism is selection of pointer states, not one history from a bundle.
>>>>>>>
>>>>>>> Bruce
>>>>>>>
>>>>>>
>>>>>>  Histories are (hidden) states. 
>>>>>>
>>>>>
>>>>> It becomes obvious that you don't really understand consistent 
>>>>> histories, either.
>>>>>
>>>>> Bruce 
>>>>>
>>>>
>>>> I've never once mentioned *consistent histories*, only *sum over 
>>>> histories*.
>>>>
>>>
>>> Inconsistent histories?
>>>  
>>>
>>>> (Did you watch the lecture by Fay Dowker?)
>>>>
>>>
>>> No, I don't watch utube videos. 
>>>
>>> Pointer states [ https://arxiv.org/abs/1508.04101 ] can best be 
>>>> understood as related to histories via the *Reflective Path Integral* 
>>>> interpretation of the EPR experiment.
>>>>
>>>
>>> Your arxiv references do not support your case. Reverse causation, as it 
>>> seems to be required in your account, is simply a nonsense. Huw Price lost 
>>> the plot a long time ago.
>>>
>>> There is no competition between the different paths between the initial 
>>> and final state -- which is what is used to calculate probabilities in the 
>>> path integral approach. So there is no Darwinian (or other) selection of 
>>> one such path over others. Quantum Darwinism is about something quite 
>>> different. Even Wikipedia agrees! Read Zurek's papers on this.
>>>
>>> Bruce
>>>
>>  
>>
>> OK. As Kay Dowker stated in her presentation: The path integral 
>> interpretation is still under development.
>>
>
> As has been pointed out, path integrals are a calculational tool, not an 
> interpretation.
>



Oh,* that* again. It's like Groundhog Day (the movie).




 
>
>> My (retrocausal) version of Darwinian selection w.r.t. multiple histories 
>> <https://en.wikipedia.org/wiki/Multiple_histories> *is* *the next 
>> development.*
>>
>
> I see, it is not actually a coherent proposition at the moment.......
>
> Bruce
>



Coherency is overrated.

- pt 

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