On Tuesday, October 15, 2019 at 10:28:09 AM UTC-5, Lawrence Crowell wrote:
>
> On Tuesday, October 15, 2019 at 6:08:27 AM UTC-5, Philip Thrift wrote:
>>
>>
>>
>> On Tuesday, October 15, 2019 at 6:02:15 AM UTC-5, Philip Thrift wrote:
>>>
>>>
>>>
>>> On Tuesday, October 15, 2019 at 5:48:58 AM UTC-5, Lawrence Crowell wrote:
>>>>
>>>> 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 
>>>>
>>>
>>> Path integrals or histories are  not eve brought up in Sean Carroll's 
>>> book (a search of the text shows).
>>>
>>> So they not present in any way in MWI.
>>>
>>> MWI (in Sean's mathematical formulation) is contrary to the path 
>>> integral, because histories (as you mention above) are simply not worlds 
>>> (in Sean's formulation).
>>>
>>> @philipthrift 
>>>
>>
>>
>> Also see Feynman's Meaning of Probabilities in QM paper.
>>
>> But there are no probabilities in MWI.
>>
>> You can't take a probabilistic theory and gloss it onto MWI.
>>
>> (like putting lipstick on a pig)
>>
>> @philipthrift 
>>
>
> Carroll and Sebens who a consistency with Born rule and MWI. Born rule is 
> about a spectrum of observable according to probability amplitudes. MWI 
> just does not assign a local probability of a measurement in quite the way 
> a collapse type interpretation does.
>
> LC 
>


Carroll himself said if you want a stochastic theory, then one world will 
do.

There is no probability theory that applies to Many Worlds that isn't 
nonsense.

@philipthrift 

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