SpaceTiger said:
There's no need for that. Please address the above points in the context of your model, even if there's no math. If you need to cut parts from or refer to other posts, that's fine. Your posts in this thread so far contain only one nitpick of the standard model (based on very sketchy observations, no lses) and a vague allusion to how you can explain the CMB acoustic oscillations. Obviously, that's not very satisfying.
In my model (which assumes an infinite Steady State universe), the virtual pairs of the quantum vacuum are polarized by the presence of matter, with antiparticles preferentially orient toward the dominant mass. In the standard model, particles and antiparticles are assumed to have equivalent gravitational mass, but that has never been experimentally demonstrated. A crucial experiment of CERN's Athena project will measure the gravitational infall rate of neutral antihydrogen, once the team has gotten past the hurdles of trapping and cooling the component particles - no small feat.
This vacuum polarization (arising from differential in gravitational infall) results in densification of the vacuum field, since as the antiparticles are preferentially oriented toward the dominant mass of matter, their partner particles are oriented outward from the dominant mass, presenting a unified front to attract and orient the antiparticles of pairs further out. This self-attractive gravitational effect does not result in collapse of the vacuum field, because the fermionic behavior of the particles and antiparticles generate an opposing pressure as they progressively resist being crowded toward the same quantum state (per the Pauli exclusion principle). The PEP pressure and the gravitational attraction are everywhere in dynamical balance to 120 OOM, explaining why the universe has not collapsed to a few thousand kilometers under the gravitational energy of the vacuum fields. The fact that the vacuum energy is so finely balanced is proof that both the pressure and the gravitational energy are aspects of the same field. If the pressure (cosmological constant if you prefer) and gravitational energy of the quantum vacuum were not features of the very same field, it would be impossible to explain the exquisite fine-tuning, and any little imbalance in the contributing fields would have long ago have caused the universe to either collapse or disintegrate.
Now for non-cosmological redshift in this model. The vacuum fields are the aether through which EM waves propagate. Einstein needed a dynamical gravitational aether to model GR, and he admitted that an EM aether was essential for the transmission of light. The problem was that he couldn't accommodate a dynamical EM aether in GR so he punted and said that although the EM aether must exist, it can have no sensible properties. In my model, the gravitational aether and the EM aether are one and the same. EM waves traversing the aether (the EM fields of the quantum vacuum) do not get a free ride. They interact with the fields and lose energy in the process. The more energetic the EM (higher frequency), the more interactions, and the more they will be slowed and redshifted, so there is a level of frequency-dependance in the model. I expect for example that gamma rays will be slowed and redshifted more than infrared, proportional to the frequency difference. If light interacts with the aether, light coming from sufficiently far away will ultimately be redshifted into indetectability. This is analagous to how AC current can be rectified and smoothed into a DC signal which contributes to the ground state of the circuit, but is no longer sensible as AC. EM of a sufficiently long wavelength is no longer sensible to us as EM. This redshifting mechanism moots Olber's Paradox as an objection to an infinite universe, since the EM from objects sufficiently far away is redshifted into undetectability. It cannot be differentiated from the ground state of the vacuum.
Now to the CMB. The CMB is simply the average temperature of the quantum vacuum - the sum of all the energy contributions from all the sources in the visible universe. Eddington calculated this temperature to be 3K in 1926 and later refined it to 2.8K which was pretty astute. Penzias and Wilson confirmed this prediction closely in 1965, and it has since been measured to be very close to Eddington's 2.8K. The CMB happens to be a fine experimental confirmation for a prediction based on a steady state universe. Gamow in his book "Creation of the Universe" had predicted that the CMB resulting from the Big Bang would be 50K. Interestingly, the Penzias and Wilson result was trumpeted as a successful confirmation for Gamow's BB model, not for Eddington's.
As to the anisotropies of the CMB as seen in WMAP data: These anisotropies are due to our motions relative to the vacuum fields, which are a semi-Machian reference frame. The motion of the MW gives us the large dipole anisotropy. Smaller anisotropies arise from the rotation of the MW, the Sun's motion through the galactic arm, and the motion of the Earth (and WMAP at L2) around the sun. If my model is correct, the gross features of the WMAP
2 data will agree with WMAP
1 results, but the small-angle anisotropies will not agree. This is because the small-angle anisotropies are artifacts of the movement of the WMAP probe relative to the vacuum fields.
Even the smallest-angle anisotropies in the WMAP data cover immense areas of space when projected back to the era of recombination. These areas are so large that they cannot possibly have conspired to change between years one and two. I predict that there are significant differences in the small-angle anisotropies between the data sets of the first two years, and that the changes will ultimately be found to be due to the orientation of the WMAP detectors relative to WMAPs motion through the vacuum field. In other words, the temperature measured in a particular spot in the celestial background is a sum of all the motions I mentioned above relative to the vacuum field plus the orientation of the detectors with respect to those motions. Higher temperatures in the forward direction and lower temperatures facing away from the direction of motion.
As for the "nitpick" about large-scale structure and high metallicity in the very early universe, some very smart people have been studying and publishing about this. I have cited many of these papers in earlier threads. The Standard Model, being time-limited, can be constrained by things like accretion rates of stars, galaxies, and black holes, the evolution of metallicity, mass budget, etc which is why these authors are interested. They seem to be serious folks, not nitpickers, and you can bet that the observational astronomers among them are already clamoring to reserve time on the LBT and the Webb to push observations far past z=6.5.
http://cosmos.as.arizona.edu/~thompson/pubdb/docs/freudling03a.pdf
http://cosmos.as.arizona.edu/~thompson/pubdb/docs/barth03a.pdf
http://citebase.eprints.org/cgi-bin/fulltext?format=application/pdf&identifier=oai%3AarXiv.org%3Aastro-ph%2F0112075
http://citebase.eprints.org/cgi-bin/fulltext?format=application/pdf&identifier=oai%3AarXiv.org%3Aastro-ph%2F0205143
http://citebase.eprints.org/cgi-bin/citations?id=oai%3AarXiv%2Eorg%3Aastro%2Dph%2F0311008