Hi Brent and Everything List Members,

    Let me start over and focus on the sequencing of OMs. I argue that the 
Schrodinger Equation does not work to generate a sequencing of Observer moments 
for multiple interacting observers because it assumes a physically unreal 
notion of time, the Newtonian Absolute time which is disallowed by the 
experimentally verified theory of general relativity. I will concede that I 
might be mistaken in my claim that the complex valuation of the observables 
(or, in the state vector formalism, the amplitudes) nor the hermiticity will 
generate a natural or well ordering that can be used to induced an a priori 
sequencing of the OMs, but I would like to see an argument that it does. Is 
there one? The paper by Ischam argues that there is not... 
    I see this problem of OM sequencing as separate from the ideas about clocks 
since clocks are a classical concept that depends, in a QM universe, on 
decoherence or something similar to overcome the effects of the HUP on its 
hands.

Onward!

Stephen

From: meekerdb 
Sent: Monday, May 09, 2011 8:04 PM
To: everything-list@googlegroups.com 
Subject: Re: Against the Doomsday hypothesis
On 5/9/2011 3:22 PM, Stephen Paul King wrote: 
  Hi Brent,


  From: meekerdb 
  Sent: Monday, May 09, 2011 12:17 PM
  To: everything-list@googlegroups.com 
  Subject: Re: Against the Doomsday hypothesis
  On 5/8/2011 10:22 PM, Stephen Paul King wrote: 
    Hi Bent,


    From: meekerdb 
    Sent: Monday, May 09, 2011 12:31 AM
    To: everything-list@googlegroups.com 
    Subject: Re: Against the Doomsday hypothesis
    On 5/8/2011 9:19 PM, Stephen Paul King wrote:
    > Hi Brent,
    >     No, the Newtonian case would be such that the logical 
    > non-contradiction requirement would be trivial as the number of 
    > physical alternatives that could occur next per state is one, this 
    > generates a one to one to one to one to one ... type of sequencing. 
    > There is no “choice” in the Newtonian case.

    And hence no measure problem.

    [SPK]
        I agree. But the universe we experience is not Newtonian...
        

    > On the other hand, in QM we have a clear example of irreducible and 
    > non-trivial alternatives that could occur next per state. IN QM, 
    > observables are defined in terms of complex valued amplitudes which do 
    > not have a well ordering as Real numbered valuations do.

    No, observables are defined by Hermitean operators which have real 
    eigenvalues.  The Hamiltonian generates time evolution.

    [SPK]
        I am sorry but you are wrong. The Hamiltonian generation of time 
evolution is only known for the non-relativistic version of QM, simple cases of 
relativistic particle dynamics and quantum field theory as currently defined. 
These use the absolute time of Newton. It is well known that the Newtonian 
version of time is disallowed by General Relativity. Chris Isham discuses this 
here: http://arxiv.org/abs/grqc/9210011
    “The problem of time in quantum gravity is deeply connected with the 
special role as-
    signed to temporal concepts in standard theories of physics. In particular, 
in Newtonian
    physics, time—the parameter with respect to which change is manifest—is 
external to
    the system itself. This is reflected in the special status of time in 
conventional quantum
    theory:”

  I'm well aware of the problem of time in quantum gravity.  But I don't think 
you need to consider relativistic QFT and solve the problem of quantum gravity 
just to have examples of "non-trivial alternatives that could occur".  I don't 
see the relevance to ordering OMs.  


  [SPKnew]
      But it is the same problem! If our notion of OMs is not related to the 
content of observations involved in such things as “inertial reference frames” 
and the general covariance of physical laws, what is the point of OMs?

       The Hermitean operators only requires that the observed “pointer bases” 
are Real numbers. In other words, the Hermiticity requirement only applies to 
the outcomes of measurements, it does not pre-order the measurements. 

  No, but they are not unordered because the wave-function is complex valued as 
you implied.  The observables, which are presumably the content of OMs are real 
valued and would be ordered by, for example, reading a clock.

  [SPK] 
      Did you actually read what I wrote? I was explicit. There was no 
implication that “they are not unordered because the wave-function is complex 
valued“, maybe I need to be even more clear and explicit. The Hermiticity 
requirement of observables DOES NOT GENERATE A WELL ORDER. Can you read that? 
The fact that each measurement is required to manifest as some Real number does 
not sequentially map the measurements into the Real line. 
      I welcome you to show otherwise.


What you wrote was." On the other hand, in QM we have a clear example of 
irreducible and non-trivial alternatives that could occur next per state .IN 
QM, observables are defined in terms of complex valued amplitudes which do not 
have a well ordering as Real numbered valuations do."



    Thus it does not lend itself to a well ordering that can be attributed to a 
dimension of time in the sense of a unique map to the Positive Reals. I am 
truly surprised that this is not well known!

  It is well know that time is not an operator in QM.  Physical time (as 
opposed to coordinate time) has to be introduced by some physical "clock".

  [SPK] 
      But “duration” can be defined as an operator that is the conjugate to 
energy. 

Look as Isham's discussion of eqn 2.1.5.  A duration operator is ruled out.


  That is a different issue. The main problem here is that the restrictions 
that general covariance places on the topology of space-time is such that our 
notion of clocks breaks down when subject to the Heisenberg uncertainty 
principle. To know exactly where the hands of the clock (or physical 
equivalent) is subject to the restrictions of the HUP. This is well trodden 
ground...


You don't need to invoke covariance or spacetime topology to see that a real 
clock must have some probability of running backwards.

Brent

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