> On 10 Jul 2021, at 21:45, 'Brent Meeker' via Everything List 
> <[email protected]> wrote:
> 
> 
> 
> On 7/10/2021 1:48 AM, Bruno Marchal wrote:
>> 
>>> On 6 Jul 2021, at 16:45, Tomas Pales <[email protected] 
>>> <mailto:[email protected]>> wrote:
>>> 
>>> 
>>> On Tuesday, July 6, 2021 at 10:28:11 AM UTC+2 Bruno Marchal wrote:
>>> 
>>>> On 3 Jul 2021, at 14:13, Tomas Pales <[email protected] 
>>>> <applewebdata://04132C56-3699-4002-9E23-EA3E9A85FE7D>> wrote:
>>>> Can't there be a machine that computes gravitational interaction with 
>>>> gravitational constant 6.674 x 10 to the -11 up until some time t and then 
>>>> continues the computation with gravitational constant 5 x 10 to the -11, 
>>>> or just halts? That would be an instability or cessation of gravitational 
>>>> law.
>>> 
>>> Yes, and that exists, but such world will have a very low probability to be 
>>> accessed by any observer, due to the fact that, below our mechanist 
>>> substitution level, all such theories intervene.
>>> 
>>> How low is this probability? Is it maybe as low as the probability that my 
>>> whole body quantum-tunnels through a wall?
>> 
>> Yes.
>> 
>> 
>> 
>>> 
>>> What does it mean that "below our mechanist substitution level, all such 
>>> theories intervene”?
>> 
>> 
>> If your consciousness does not require some details: like the position of an 
>> electron of some atom in some neurotransmitter (say), then it will be 
>> associate as much with your brain and that election here, and with you brain 
>> and that electron there, and if you don’t measure the position of that 
>> electron, the two histories can interfere statistically.
> What would it mean to measure the state of your own brain?

To encode the relevant information such that I survive the copy/reconstitution. 
The possibility of this is assumed in the YD part of the YD+CT.
YD = “Yes doctor”, and CT = Church’s Thesis (or Church-Turing’s thesis).

Bruno




> 
> Brent
> 
>> 
>> An electronic orbital is such a map: it tells you where you can find the 
>> electron in your most probable computational histories.
>> 
>> Bruno 
>> 
>> 
>> 
>> 
>>> 
>>> 
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