Density Profiles of Collapsed Rotating Massive Stars Favor Long Gamma-Ray Bursts

• Published in: Astrophysical journal. Letters Vol. 944; no. 2; p. L38
• Main Authors: Halevi, Goni, Wu, Belinda, Mösta, Philipp, Gottlieb, Ore, Tchekhovskoy, Alexander, Aguilera-Dena, David R.
• Format: Journal Article
• Language: English
• Published: Austin The American Astronomical Society 01.02.2023; IOP Publishing
• Subjects: Astronomical models; Black holes; Core-collapse supernovae; Density; Gamma ray astronomy; Gamma ray bursts; Gamma rays; General relativity; Hydrodynamical simulations; Jets; Massive stars; Metallicity; Modelling; Neutron stars; Progenitors (astrophysics); Source code; Space telescopes; Stellar mass black holes; Stellar models; Stellar rotation
• ISSN: 2041-8205; 2041-8213
• DOI: 10.3847/2041-8213/acb702

Abstract Long-duration gamma-ray bursts (lGRBs) originate in relativistic collimated outflows—jets—that drill their way out of collapsing massive stars. Accurately modeling this process requires realistic stellar profiles for the jets to propagate through and break out of. Most previous studies have used simple power laws or pre-collapse models for massive stars. However, the relevant stellar profile for lGRB models is in fact that of a star after its core has collapsed to form a compact object. To self-consistently compute such a stellar profile, we use the open-source code GR1D to simulate the core-collapse process for a suite of low-metallicity rotating massive stellar progenitors that have undergone chemically homogeneous evolution. Our models span a range of zero-age main-sequence (ZAMS) masses: M ZAMS = 13, 18, 21, 25, 35, 40, and 45 M ☉ . All of these models, at the onset of core-collapse, feature steep density profiles, ρ ∝ r − α , with α ≈ 2.5, which would result in jets that are inconsistent with lGRB observables. We follow the collapses of four of the seven models until they form black holes (BHs) and the other three models until they form proto-neutron stars (PNSs). We find, across all models, that the density profile outside the newly formed BH or PNS is well represented by a flatter power law with α ≈ 1.35–1.55. Such flat density profiles are conducive to the successful formation and breakout of BH-powered jets and are, in fact, required to reproduce observable properties of lGRBs. Future models of lGRBs should be initialized with shallower post-collapse stellar profiles, like those presented here, instead of the much steeper pre-collapse profiles that are typically used.