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Statistical properties of the combined emission of a population of discrete sources: astrophysical implications

2003/12/31 by M. Gilfanov, H. J. Grimm, H-J. Grimm +1 · 2 citations
Physics and Astronomy · #Cosmology and Gravitation Theories #Galaxies: Formation, Evolution, Phenomena #High-Energy Particle Collisions Research #astro-ph

paper · pdf · doi:10.1111/j.1365-2966.2004.07874.x

published as Mon.Not.Roy.Astron.Soc. 351 (2004) 1365 · MNRAS, accepted for publication

arxiv created 2004/03/26 · openalex publication_date 2004/07/01 · arxiv updated 2009/12/01 · openalex created_date 2025/10/10 · openalex updated_date 2026/07/28

Abstract

We study the statistical properties of the combined emission of a population of discrete sources (for example, the X-ray emission of a galaxy due to its population of X-ray binaries). Namely, we consider the dependence of their total luminosity and of the fractional rmstot of their variability on the number of sources n or, equivalently, on the normalization of the luminosity function. We show that, as a result of small number statistics, a regime exists in which Ltot grows non-linearly with n, in apparent contradiction with the seemingly obvious prediction . In this non-linear regime, rmstot decreases with n significantly more slowly than expected from the averaging law. For example, for a power-law luminosity function with a slope of α= 3/2, in the non-linear regime, Ltot∝n2 and rmstot does not depend at all on the number of sources n. Only in the limit of n→∞ do these quantities behave as intuitively expected, Ltot∝n and . We give exact solutions and derive convenient analytical approximations for Ltot and rmstot. Using the total X-ray luminosity of a galaxy due to its X-ray binary population as an example, we show that the LX–star formation rate and LX–M* relations predicted from the respective ‘universal’ luminosity functions of high- and low-mass X-ray binaries are in good agreement with observations. Although caused by small number statistics, the non-linear regime in these examples extends as far as SFR ≲ 4–5 M⊙ yr−1 and log(M*/M⊙) ≲ 10.0–10.5, respectively.

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