- #36
Fra
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- 618
I don't know half as much as Marcus on these things but I read some of their papers and here are some of my reflections...
A general problem is that of counting geometries (or counting anything). Ie. one asks what is the set of possible geometries. The set of all possible geometries can be called a microstructure. And each geometry is a microstate.
If we also on that set can find a measure that assigns probability amplitudes between any two microstates, then one would expect that the result from "diffusion" or random walking from an arbitrary initial condition, should follow certain dynamics at the statistical level.
I think there is an ambigouity in their choice of this set of geometries and the action measures. If I were to dig into CDT these two points is what I'd try to improve.
They seem to want to give the impression that their way of counting geometries since it's based on random sampling over all possible geometries are universal and fair. But that's exactly the deceptive part. This problem exists also in classical stat mech.
What I am looking for is taking the process, that generates/constructs the sampling space seriously... and look for the physics in it. I think matter may come out of that, because matter may be the relational references that is missing to make this more conceptually consistent. Because in effect matter could as I like to think of it quality as "observers". And the logic of constructing and counting geometries may must IMO be attached to observers.
So while I like the statistical approach in CDT, the poins where I can't help disliking it's arguments are possibly also the points which should resolve once matter is incorporated.
If something like that will come out of CDT, I would be vary interested.
This seems to be from 2005 rather than 1995, from "Reconstructing the Universe"
J. Ambjorn, J. Jurkiewicz (U. Krakow), R. Loll (U. Utrecht)
http://arxiv.org/abs/hep-th/0505154
/Fredrik
oldman said:What "microscopic components" do they mean? Not their simplices, I hope, which are just a calculationional tool, as I read you:
A general problem is that of counting geometries (or counting anything). Ie. one asks what is the set of possible geometries. The set of all possible geometries can be called a microstructure. And each geometry is a microstate.
If we also on that set can find a measure that assigns probability amplitudes between any two microstates, then one would expect that the result from "diffusion" or random walking from an arbitrary initial condition, should follow certain dynamics at the statistical level.
I think there is an ambigouity in their choice of this set of geometries and the action measures. If I were to dig into CDT these two points is what I'd try to improve.
They seem to want to give the impression that their way of counting geometries since it's based on random sampling over all possible geometries are universal and fair. But that's exactly the deceptive part. This problem exists also in classical stat mech.
What I am looking for is taking the process, that generates/constructs the sampling space seriously... and look for the physics in it. I think matter may come out of that, because matter may be the relational references that is missing to make this more conceptually consistent. Because in effect matter could as I like to think of it quality as "observers". And the logic of constructing and counting geometries may must IMO be attached to observers.
So while I like the statistical approach in CDT, the poins where I can't help disliking it's arguments are possibly also the points which should resolve once matter is incorporated.
If something like that will come out of CDT, I would be vary interested.
oldman said:"...we are in the process of developing new and more refined methods to probe the geometry of the model further, and which eventuallyshould allow us to test aspects related to its local “transverse” degrees offreedom, the gravitons. We invite and challenge our readers to find such tests ina truly background-independent formalism of quantum gravity."
This seems to be from 2005 rather than 1995, from "Reconstructing the Universe"
J. Ambjorn, J. Jurkiewicz (U. Krakow), R. Loll (U. Utrecht)
http://arxiv.org/abs/hep-th/0505154
/Fredrik