^1,2Daohai Li,²Alexander J. Mustill,^2,3Melvyn B. Davies
The Astrophysical Journal 924, 61 Open Access Link to Article [DOI 10.3847/1538-4357/ac33a8]
¹Department of Astronomy Beijing Normal University, No.19, Xinjiekouwai Street, Haidian District, Beijing, 100875, People’s Republic of China; lidaohai@gmail.com, lidaohai@bnu.edu.cn
²Lund Observatory Department of Astronomy and Theoretical Physics Lund University, Box 43, SE-221 00 Lund, Sweden
³Centre for Mathematical Sciences Lund University, Box 118, SE-221 00 Lund, Sweden

White dwarfs (WDs) often show metal lines in their spectra, indicating accretion of asteroidal material. Our Sun is to become a WD in several gigayears. Here, we examine how the solar WD accretes from the three major small body populations: the main belt asteroids (MBAs), Jovian Trojan asteroids (JTAs), and trans-Neptunian objects (TNOs). Owing to the solar mass loss during the giant branch, 40% of the JTAs are lost but the vast majority of MBAs and TNOs survive. During the WD phase, objects from all three populations are sporadically scattered onto the WD, implying ongoing accretion. For young cooling ages ≲100 Myr, accretion of MBAs predominates; our predicted accretion rate ∼106 g s−1 falls short of observations by two orders of magnitude. On gigayear timescales, thanks to the consumption of the TNOs that kicks in ≳100 Myr, the rate oscillates around 106–107 g s−1 until several gigayears and drops to ∼105 g s−1 at 10 Gyr. Our solar WD accretion rate from 1 Gyr and beyond agrees well with those of the extrasolar WDs. We show that for the solar WD, the accretion source region evolves in an inside-out pattern. Moreover, in a realistic small body population with individual sizes covering a wide range as WD pollutants, the accretion is dictated by the largest objects. As a consequence, the accretion rate is lower by an order of magnitude than that from a population of bodies of a uniform size and the same total mass and shows greater scatter.