> On 21 Jun 2018, at 22:12, Brent Meeker <[email protected]> wrote:
> 
> 
> 
> On 6/21/2018 2:13 AM, Bruno Marchal wrote:
>> 
>>> On 20 Jun 2018, at 00:28, Brent Meeker <[email protected] 
>>> <mailto:[email protected]>> wrote:
>>> 
>>> 
>>> 
>>> On 6/19/2018 7:25 AM, Bruno Marchal wrote:
>>>> 
>>>>> On 16 Jun 2018, at 22:41, Brent Meeker <[email protected] 
>>>>> <mailto:[email protected]>> wrote:
>>>>> 
>>>>> 
>>>>> 
>>>>> On 6/16/2018 10:16 AM, John Clark wrote:
>>>>>> ​> ​ Another universe comes into existence when Joe the Plumber 
>>>>>> performs, say, a spin measurement.
>>>>>> 
>>>>>> But a measurement (whatever in the world that means) does not need to be 
>>>>>> made and there is nothing special about Joe, if Everett is right the 
>>>>>> same thing happens every time an electron in Joe's skin encounters a 
>>>>>> photon, or for that matter whenever an electron anywhere encounters 
>>>>>> anything.
>>>>> 
>>>>> That's where MWI gets fuzzy. 
>>>> 
>>>> Not more than QM itself. We can define a world by a branch of the universe 
>>>> wave. But such world will be “world” only as part of a personal history. 
>>>> Everett disagrees, but his “relative state” is a better wording than 
>>>> “many-worlds” which is often confusing.
>>>> 
>>>> 
>>>> 
>>>>> Do all the submicroscopic events that make to macroscopic difference 
>>>>> create different worlds?  That can't be right because "worlds" are 
>>>>> classical things.  So the Heisenberg but problem seems to reappear in 
>>>>> different form.
>>>> 
>>>> Heisenberg cut disappear, it is just that worlds differentiate from our 
>>>> perspective when they make difference for us, like when they can no more 
>>>> interfere. There is no cut, only the quantum wave (in the Schroedinger 
>>>> picture) and relative state related to macroscopic irreversibility, which 
>>>> needs only the classical chaos to be irreversible FAPP. Histories are 
>>>> internal things, already a form of first person plural notion. 
>>> 
>>> Right.  But how FAPP does it have to be, how irreversible, in order that it 
>>> constitutes a conscious distinct state?  That's how the Heisenberg cut 
>>> problem reappears at a different level.
>> 
>> Very quickly, like when you mix milk in the coffee. Pure statistics theory 
>> provides the numbers, like when we can use Gauss e^(-x^2) instead of Pascal 
>> triangle. You don’t need 0 on the diagonal, only tiny numbers.
> 
> I think you mean OFF the diagonal. 

Indeed.



> But how do you know you only need tiny numbers, and how tiny?  I have thought 
> that perhaps there should be a smallest non-zero unit of probability; but it 
> has been pointed out that even tiny numbers may add up when the density 
> matrix is transformed to some other basis.

It is just that the numbers are tiny only from your (3p) personal points of 
view. You brain needs to be enough of a mixture for consciousness to 
differentiate into universal machine (relative) state. In the case (which I 
doubt) that the brain is a quantum computer, we would be able to exploit the 
numbers which are not tiny in the relevant base to exploit quantum computing 
ability.





> 
>> You don’t need purely orthogonal state, the big numbers and classical chaos 
>> will lead to the right quasi classical phenomenology,
> 
> So you say.  But that requires a theory of "phenomenology", i.e. a theory of 
> how perception is realized.

But I extract the quantum from such a phenomenology. Perception is mainly 
[a]<a>p with [a] designing a variant of the logic of self-reference G, or G*.

It is provably realised in all models of the consistent extensions of very 
elementary arithmetic.

(You might need to study some books on self-reference (the provability logic) 
to get the point).

Bruno




> 
> Brent
> 
>> for most relative observers. We don’t need to kill all white rabbits, just 
>> to make them relatively rare. 
>> 
>> Bruno
>> 
>> 
>> 
>> 
>>> 
>>> Brent
>>> 
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