On Tuesday, October 15, 2019 at 2:24:10 AM UTC-5, Philip Thrift wrote:
>
>
>
> On Monday, October 14, 2019 at 6:52:24 PM UTC-5, Lawrence Crowell wrote:
>>
>> On Monday, October 14, 2019 at 4:44:42 PM UTC-5, Bruce wrote:
>>>
>>> On Tue, Oct 15, 2019 at 5:38 AM Philip Thrift <[email protected]> 
>>> wrote:
>>>
>>>> On Monday, October 14, 2019 at 1:20:39 PM UTC-5, Brent wrote:
>>>>>
>>>>> Part of the dislike of the MWI is that its proponents assume a purity 
>>>>> that is not an evident virtue of the intepretation.  For example, 
>>>>> interpreting the squared amplitudes as probabilities seems to be assumed, 
>>>>> along with the existence of the preferred basis in which the amplitudes 
>>>>> are 
>>>>> defined.  Together these are almost the same as CI.  If you ask 
>>>>> "probabilities of what?" in MWI the answer can't be probability of 
>>>>> existing 
>>>>> because MWI has committed to all solutions, however improbable, existing. 
>>>>>  
>>>>> So it becomes probability of finding yourself in a particular 
>>>>> world...which 
>>>>> depends on a theory of consciousness and seems to regress to von Neumann 
>>>>> and Wigner.
>>>>>
>>>>> Zurek's envariance attempts to answer these questions and provide a 
>>>>> justification for preferred bases and what probability refers to.  But 
>>>>> notice that to the extent he succeeds he is justifying taking a simple 
>>>>> probabilistic view and saying one of those preferred states happens and 
>>>>> the 
>>>>> others don't.
>>>>>
>>>>> Brent
>>>>>
>>>>>
>>>>>
>>>> In the single-particle double-slit experiment*, an observer could see a 
>>>> dot appear anywhere on a screen where path interference does not reduce 
>>>> the 
>>>> probability to zero. So with the literal many-world-branching theory, how 
>>>> many different worlds are produced, each on with its own observer seeing a 
>>>> dot on the screen?
>>>>
>>>
>>> According to MWI, an infinite number. Each world will have the dot at a 
>>> different place on the screen.
>>>
>>> Bruce
>>>
>>
>> What you say may open up a bit of a hole or snag in MWI. This is 
>> something I have been pondering some since Carroll's popularization. If MWI 
>> fundamentally preserves unitarity by splitting off worlds then localization 
>> of a measurement is an illusion.Consider a particle measured somewhere on a 
>> path from x and x'.  The path integral and the nonlocality of paths is a 
>> sum over all possible measurements in all space containing x and x', then 
>> there must be a continuum of possible worlds splitting off. If the operator 
>> has a continuum of eigenvalues *x*|x> = x|x> there must then be a 
>> continuum of possible worlds if there is indeed no fundamental localization 
>> with a measurement. This is not just infinite, but uncountably infinite.
>>
>> This is different from how decoherence maintains unitarity and conserves 
>> qubits. There a local interaction occurs that induces quantum phase to 
>> enter into a set of ancillary states or reservoir of states. Then we can 
>> consider quantum states as finite, but unbounded from above, so that local 
>> observations and measurements are possible. 
>>
>> This does seem to run into some oddities that either need to be worked 
>> out or that might indicate some gap in MWI. The persistence of nonlocality 
>> in MWI is interesting for possible quantum gravitation work. In that case I 
>> can think of maybe a way around this, where this uncountably infinite set 
>> of g_{ij} configurations, or Ψ[g_{ij}], can be identified with "exotic" 
>> manifolds that are removed. It is less clear how this can happen with 
>> ordinary quantum fields that have local realizations.
>>
>> LC
>>
>
>
>
> To mix an analysis (or a theory) of the path integral with an analysis (or 
> a theory) of MWI is mixing two fundamentally contradictory frameworks that 
> only leads to confusion.
>
> @philipthrift 
>

I am thinking of a path integral as most physicists do, which is an action 
principle that is a sum over amplitudes or histories. You are thinking 
according to the quantum interpretation of Dowker and others, which has 
auxiliary postulates or assumptions.

LC 

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