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In article <[EMAIL PROTECTED]>, Ralph Hartley <[EMAIL PROTECTED]> writes: > An interesting article: > > http://www.nytimes.com/2003/10/09/science/09COSM.htm Just a comment, since it might not be obvious to all readers, and since as usual this will probably be painted by much of the media as a "sensation" which "shakes the foundations of physics" and possibly even "challenges Einstein". The first I'll agree with---if the hunches turn out to be true. The second and third, certainly not. The range of "standard cosmological models", i.e. those based on General Relativity and or those generally referred to as Friedmann-Lemaitre models, have something called the curvature parameter. This, however, refers to the LOCAL curvature, not the global topology, about which such models say nothing. (In other words, with classical cosmological tests (i.e. working out the dependence of an observable quantity on redshift and fitting the cosmological parameters to the observations), one can't determine the global topology---one needs other methods, such as analysing the CMB.) The "local" curvature can be the same everywhere---and has to be if the model satisfies the cosmological principle. An analogy is a cylinder: its local curvature is 0, i.e. the same as a plane. Its global topology, however, is obviously different. One can see this via the fact that one can roll up a sheet of paper to make a cylinder without having to stretch, tear, fold or wrinkle it. In more than two dimensions, things are more complicated, but the principle is the same: a given local curvature can exist in more than one global topology.
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