> On 4 Dec 2018, at 09:25, Philip Thrift <[email protected]> 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 <[email protected] <javascript:>> 
>>> 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, [email protected] <> 
>>>>> 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”:

… where Omnès added “time to be irrational” ...



> 
> 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.

"5.”  follows from mechanism as a first person view. No need of Omnès 
mysterious selection.

Bruno



> 
> See the Wheeler-Feynman computer:
> [ 
> https://codicalist.wordpress.com/2018/09/25/retrosignaling-in-the-quantum-substrate/
>  ]
> 
> - pt
> 
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