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The Initial Mass Function Based on the Full-sky 20-pc Census of \\(\\sim\\)3,600 Stars and Brown Dwarfs
The Initial Mass Function Based on the Full-sky 20-pc Census of \\(\\sim\\)3,600 Stars and Brown Dwarfs
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The Initial Mass Function Based on the Full-sky 20-pc Census of \\(\\sim\\)3,600 Stars and Brown Dwarfs
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The Initial Mass Function Based on the Full-sky 20-pc Census of \\(\\sim\\)3,600 Stars and Brown Dwarfs
The Initial Mass Function Based on the Full-sky 20-pc Census of \\(\\sim\\)3,600 Stars and Brown Dwarfs

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The Initial Mass Function Based on the Full-sky 20-pc Census of \\(\\sim\\)3,600 Stars and Brown Dwarfs
The Initial Mass Function Based on the Full-sky 20-pc Census of \\(\\sim\\)3,600 Stars and Brown Dwarfs
Paper

The Initial Mass Function Based on the Full-sky 20-pc Census of \\(\\sim\\)3,600 Stars and Brown Dwarfs

Ma
2023
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Overview
A complete accounting of nearby objects -- from the highest-mass white dwarf progenitors down to low-mass brown dwarfs -- is now possible, thanks to an almost complete set of trigonometric parallax determinations from Gaia, ground-based surveys, and Spitzer follow-up. We create a census of objects within a Sun-centered sphere of 20-pc radius and check published literature to decompose each binary or higher-order system into its separate components. The result is a volume-limited census of \\(\\sim\\)3,600 individual star formation products useful in measuring the initial mass function across the stellar (\\(<8 M_\\odot\\)) and substellar (\\(\\gtrsim 5 M_{Jup}\\)) regimes. Comparing our resulting initial mass function to previous measurements shows good agreement above 0.8\\(M_\\odot\\) and a divergence at lower masses. Our 20-pc space densities are best fit with a quadripartite power law, \\(\\xi(M) = dN/dM \\propto M^{-\\alpha}\\) with long-established values of \\(\\alpha = 2.3\\) at high masses (\\(0.55 < M < 8.00 M_\\odot\\)) and \\(\\alpha = 1.3\\) at intermediate masses (\\(0.22 < M < 0.55 M_\\odot\\)), but at lower masses we find \\(\\alpha = 0.25\\) for \\(0.05 < M <0.22 M_\\odot\\) and \\(\\alpha = 0.6\\) for \\(0.01 < M < 0.05 M_\\odot\\). This implies that the rate of production as a function of decreasing mass diminishes in the low-mass star/high-mass brown dwarf regime before increasing again in the low-mass brown dwarf regime. Correcting for completeness, we find a star to brown dwarf number ratio of, currently, 4:1, and an average mass per object of 0.41 \\(M_\\odot\\).