[0809.3734] A measurement of large-scale peculiar velocities of clusters of galaxies: results and cosmological implications
Authors: | A. Kashlinsky (GSFC), F. Atrio-Barandela (U of Salamanca), D. Kocevski (UC Davis), H. Ebeling (U of Hawaii) |
Abstract: | Peculiar velocities of clusters of galaxies can be measured by studying the fluctuations in the cosmic microwave background (CMB) generated by the scattering of the microwave photons by the hot X-ray emitting gas inside clusters. While for individual clusters such measurements result in large errors, a large statistical sample of clusters allows one to study cumulative quantities dominated by the overall bulk flow of the sample with the statistical errors integrating down. We present results from such a measurement using the largest all-sky X-ray cluster catalog combined to date and the 3-year WMAP CMB data. We find a strong and coherent bulk flow on scales out to at least > 300 h^{-1} Mpc, the limit of our catalog. This flow is difficult to explain by gravitational evolution within the framework of the concordance LCDM model and may be indicative of the tilt exerted across the entire current horizon by far-away pre-inflationary inhomogeneities. |
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[0809.3734] A measurement of large-scale peculiar velociti
(This is a companion to the longer paper 0809.3733, where the authors provide more details.)
The authors claim to have detected a coherent bulk flow over a scale of at least 300 h^{-1}Mpc. While this might not be completely surprising (see 0809.4041, for example), their method leaves me baffled.
They claim to make the detection using the kinetic SZ effect. They argue as follows, as far as I understand (which is not very far). Take the CMB sky and a cluster catalogue. Remove the cosmological contribution from the CMB sky. Calculate the dipole and monopole at the location of the clusters from this subtracted sky. Now you have the thermals and kinetic SZ components, and from the dipole you identify the kinetic SZ effect, which you can use to measure the peculiar velocity of the cluster.
If their claim is true, it's important as a detection of the kinetic SZ effect at a high significance, apart from the implications for bulk flows. But there are a number of things I don't understand. One of them is: how is it possible to subtract the cosmological CMB sky from the observed one? I understand doing simulations (given a cosmological model) to assess whether something is likely or unlikely to be present in a realisation of a certain cosmology, but that does not seem to be what they are doing. They write that they use a Wiener filter (page 3 of this paper, page 12 of the longer paper), which doesn't say a lot to me.
The authors claim to have detected a coherent bulk flow over a scale of at least 300 h^{-1}Mpc. While this might not be completely surprising (see 0809.4041, for example), their method leaves me baffled.
They claim to make the detection using the kinetic SZ effect. They argue as follows, as far as I understand (which is not very far). Take the CMB sky and a cluster catalogue. Remove the cosmological contribution from the CMB sky. Calculate the dipole and monopole at the location of the clusters from this subtracted sky. Now you have the thermals and kinetic SZ components, and from the dipole you identify the kinetic SZ effect, which you can use to measure the peculiar velocity of the cluster.
If their claim is true, it's important as a detection of the kinetic SZ effect at a high significance, apart from the implications for bulk flows. But there are a number of things I don't understand. One of them is: how is it possible to subtract the cosmological CMB sky from the observed one? I understand doing simulations (given a cosmological model) to assess whether something is likely or unlikely to be present in a realisation of a certain cosmology, but that does not seem to be what they are doing. They write that they use a Wiener filter (page 3 of this paper, page 12 of the longer paper), which doesn't say a lot to me.
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[0809.3734] A measurement of large-scale peculiar velociti
Also Figure 1(f) seems to suggest we should be involved in a bulk flow of around 1500 kms^{-1}. If this were true, then presumably our own peculiar velocity would have to be quite contrived (large and aligned anti-parallel to the flow) in order to produce the CMB dipole of v < 400kms^{-1}.
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[0809.3734] A measurement of large-scale peculiar velociti
Well, the error bar is quite large. Doubling that would get you down to 500-600 km/s. In the conclusions of the longer paper, they quote the value 600-1000 km/s.
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[0809.3734] A measurement of large-scale peculiar velocitie
True. But then if you treble them you can get down to v=0. :)
Even with a bulk flow of 800kms^{-1}, which is lower than any of their data points, and assuming our peculiar velocity matched that in magnitude,
the alignment is still a bit of a problem. You'd still find a ~95% chance (I think) of our dipole being larger than it is.
Even with a bulk flow of 800kms^{-1}, which is lower than any of their data points, and assuming our peculiar velocity matched that in magnitude,
the alignment is still a bit of a problem. You'd still find a ~95% chance (I think) of our dipole being larger than it is.
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Re: [0809.3734] A measurement of large-scale peculiar veloc
I don't see your point. You only need the real value to be at the edge of the error bars at our location to be compatible with the CMB dipole, whereas getting rid of the bulk flow would require all points being at the edge.Fergus Simpson wrote:True. But then if you treble them you can get down to v=0. :)
However, I agree that there seems to be a bit of a coincidence required, in that we happen to be in a location where the flow is much smaller than the mean bulk flow (or anticorrelated with the CMB dipole).
All of this is assuming the analysis would be correct, of course...