On Tuesday, December 4, 2018 at 1:53:15 PM UTC-6, Brent wrote:
>
>
>
> On 12/4/2018 12:25 AM, Philip Thrift wrote:
>
>
>
> On Monday, December 3, 2018 at 9:00:26 PM UTC-6, Brent wrote: 
>>
>>
>>
>> On 12/3/2018 8:50 AM, Bruno Marchal wrote:
>>
>>
>> On 3 Dec 2018, at 10:35, Philip Thrift <cloud...@gmail.com> wrote:
>>
>>
>>
>> On Sunday, December 2, 2018 at 8:17:54 PM UTC-6, Brent wrote: 
>>>
>>>
>>>
>>> On 12/2/2018 5:14 PM, Philip Thrift wrote:
>>>
>>>
>>>
>>> On Sunday, December 2, 2018 at 4:25:04 PM UTC-6, Brent wrote: 
>>>>
>>>>
>>>>
>>>> On 12/2/2018 11:42 AM, Philip Thrift wrote:
>>>>
>>>>
>>>>
>>>> On Sunday, December 2, 2018 at 8:13:48 AM UTC-6, agrays...@gmail.com 
>>>> wrote: 
>>>>>
>>>>>
>>>>> *Obviously, from a one-world perspective, only one history survives 
>>>>> for a single trial. But to even grossly approach anything describable as 
>>>>> "Darwinian", you have to identify characteristics of histories which 
>>>>> contribute positively or negatively wrt surviving but I don't see an 
>>>>> inkling of that. IMO, Quantum Darwinism is at best a vacuous restatement 
>>>>> of 
>>>>> the measurement problemt; that we don't know why we get what we get. AG*
>>>>>
>>>>>>
>>>>>>
>>>>>>
>>>>
>>>> In the *sum over histories* interpretation - of the double-slit 
>>>> experiment, for example - each history carries a unit complex number - 
>>>> like 
>>>> a gene - and this gene reenforces (positively) or interferes (negatively) 
>>>> with other history's genes in the sum.
>>>>
>>>>
>>>> But I thought you said the ontology was that only one history "popped 
>>>> out of the Lottery machine"?  Here you seem to contemplate an ensemble of 
>>>> histories, all those ending at the given spot, as being real.
>>>>
>>>> Brent
>>>>
>>>
>>>
>>>
>>>
>>> All are real until all but one dies.
>>> RIP: All those losing histories.
>>>
>>>
>>> The trouble with that is the Born probability doesn't apply to 
>>> histories, it applies to results.  So your theory says nothing about the 
>>> probability of the fundamental ontologies.
>>>
>>> Brent
>>>
>>
>>
>>
>>
>>
>> The probability distribution on the space of histories is provided by the 
>> path integral. 
>>
>>
>> Except that isn't true. A probability (or probability density) is 
>> provided for a bundle of histories joining two events.  It doesn't not 
>> provide a probability of a single history.
>>
>> Brent
>>
>>
> That's why you add to that "pick any history at random from the bundle":
>
>
> But the probability didn't apply to that history.  The Born rule gave the 
> probability of the bundle.  To it is false that, "The probability 
> distribution on the space of histories is provided by the path integral." 
>
>
> 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
>
>
> See the *Wheeler-Feynman computer*:
> [ 
> https://codicalist.wordpress.com/2018/09/25/retrosignaling-in-the-quantum-substrate/
>  
> ]
>
> - p
>
>
>
 

Selection happens via quantum Darwinism. 

- pt 

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