Source counts

The source counts distribution of radio-sources from a radio-astronomical survey is the cumulative distribution of the number of sources (N) brighter than a given flux density (S). Because it is usually plotted with the log-log scale, so its distribution is also called as the log N - log S plot. It is one out of a half-dozen cosmological tests that was conceived in the 1930s to check the viability of and compare new cosmological models[1].

Early work on cataloguing radio sources had as an aim the determination of the source counts distribution to help astronomers decide between cosmological models. For a uniform distribution of radio sources at not too large redshift (i.e. in a 'steady-state, Euclidean universe') the slope of the cumulative distribution of log(N) versus log(S) would be −1.5.

Data from the early Cambridge 2C survey (published 1955) apparently implied a (log(N), log(S)) slope of nearly −3.0. This appeared to invalidate the steady state theory of Fred Hoyle, Hermann Bondi and Thomas Gold. Unfortunately many of these weaker sources were subsequently found to be due to 'confusion' (the blending of several weak sources in the side-lobes of the interferometer, to give a response like one stronger one).

By contrast, analysis from the contemporaneous Mills Cross data (by Slee and Mills) were consistent with an index of −1.5.

Later and more accurate surveys from Cambridge, 3C, 3CR, and 4C, also showed source count slopes steeper than −1.5, though by a smaller margin than 2C. This convinced some cosmologists that the steady state theory was wrong, although residual problems with confusion provided some defense for Hoyle and his colleagues.

The immediate interest in testing the steady-state theory through source-counts was reduced by the discovery of the 3K microwave background radiation in the mid 1960s, which essentially confirmed the Big-Bang model.

Later radio survey data have shown a complex picture[2][3][4] — the 3C and 4C claims appear to hold up, while at fainter levels the source counts flatten substantially below a slope of −1.5. This is now understood to reflect the effects of both density and luminosity evolution of the principal radio sources over cosmic timescales.


See also

References

  1. ↑ "Radio source counts and their interpretation" Kellermann, K. I.; Wall, J. V., Observational cosmology; Proceedings of the IAU Symposium, Beijing, People's Republic of China, Aug. 25-30, 1986
  2. ↑ http://sundog.stsci.edu/first/catalog_paper/node6.html
  3. ↑ "A Catalog of 1.4 GHz Radio Sources from the FIRST Survey" White, R. L., Becker, R. H., Helfand, D. J., & Gregg, M. D. 1997, ApJ, 475, 479
  4. ↑ "Probing the Cosmological Principle in the counts of radio galaxies at different frequencies", Bengaly, Carlos A. P.; Maartens, Roy; Santos, Mario G.; Journal of Cosmology and Astro-Particle Physics 2018(04)
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