TY - JOUR
T1 - Density Profiles of Collapsed Rotating Massive Stars Favor Long Gamma-Ray Bursts
AU - Halevi, Goni
AU - Wu, Belinda
AU - Mösta, Philipp
AU - Gottlieb, Ore
AU - Tchekhovskoy, Alexander
AU - Aguilera-Dena, David R.
N1 - Funding Information:
We thank Evan O’Connor for helpful discussions and advice about using GR1D. We also thank Jim Stone, Eliot Quataert, and Elias Most for helpful discussions, and the anonymous referee for insightful feedback on an earlier version of this manuscript. G.H. is supported in part by a National Science Foundation Graduate Research Fellowship. O.G. is supported by a CIERA Postdoctoral Fellowship. O.G. and A.T. acknowledge support from the Fermi Cycle 14 Guest Investigator program 80NSSC22K0031. A.T. was supported by NSF grant Nos. AST-2107839, AST-1815304, AST-1911080, and OAC-2031997, and NASA grant No. 80NSSC18K0565. D.R.A.-D. acknowledges support from the Stavros Niarchos Foundation (SNF) and the Hellenic Foundation for Research and Innovation (HFRI) under the 2nd Call for Action “Science and Society” “Always Strive for Excellence—Theodoros Papazoglou” (Project No. 01431). The simulations presented here were performed on computational resources that are managed and supported by Princeton Research Computing, a consortium of groups including the Princeton Institute for Computational Science and Engineering (PICSciE) and the Office of Information Technology’s High Performance Computing Center and Visualization Laboratory at Princeton University.
Funding Information:
We thank Evan O’Connor for helpful discussions and advice about using GR1D. We also thank Jim Stone, Eliot Quataert, and Elias Most for helpful discussions, and the anonymous referee for insightful feedback on an earlier version of this manuscript. G.H. is supported in part by a National Science Foundation Graduate Research Fellowship. O.G. is supported by a CIERA Postdoctoral Fellowship. O.G. and A.T. acknowledge support from the Fermi Cycle 14 Guest Investigator program 80NSSC22K0031. A.T. was supported by NSF grant Nos. AST-2107839, AST-1815304, AST-1911080, and OAC-2031997, and NASA grant No. 80NSSC18K0565. D.R.A.-D. acknowledges support from the Stavros Niarchos Foundation (SNF) and the Hellenic Foundation for Research and Innovation (HFRI) under the 2nd Call for Action “Science and Society” “Always Strive for Excellence—Theodoros Papazoglou” (Project No. 01431). The simulations presented here were performed on computational resources that are managed and supported by Princeton Research Computing, a consortium of groups including the Princeton Institute for Computational Science and Engineering (PICSciE) and the Office of Information Technology’s High Performance Computing Center and Visualization Laboratory at Princeton University.
Publisher Copyright:
© 2023. The Author(s). Published by the American Astronomical Society.
PY - 2023/2/1
Y1 - 2023/2/1
N2 - 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 45M ☉. 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.
AB - 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 45M ☉. 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.
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U2 - 10.3847/2041-8213/acb702
DO - 10.3847/2041-8213/acb702
M3 - Article
AN - SCOPUS:85148766251
SN - 2041-8205
VL - 944
JO - Astrophysical Journal Letters
JF - Astrophysical Journal Letters
IS - 2
M1 - L38
ER -