Author
Listed:
- Kritti Sharma
(California Institute of Technology)
- Vikram Ravi
(California Institute of Technology
California Institute of Technology)
- Liam Connor
(California Institute of Technology)
- Casey Law
(California Institute of Technology
California Institute of Technology)
- Stella Koch Ocker
(California Institute of Technology
The Observatories of the Carnegie Institution for Science)
- Myles Sherman
(California Institute of Technology)
- Nikita Kosogorov
(California Institute of Technology)
- Jakob Faber
(California Institute of Technology)
- Gregg Hallinan
(California Institute of Technology
California Institute of Technology)
- Charlie Harnach
(California Institute of Technology
California Institute of Technology)
- Greg Hellbourg
(California Institute of Technology
California Institute of Technology)
- Rick Hobbs
(California Institute of Technology
California Institute of Technology)
- David Hodge
(California Institute of Technology
California Institute of Technology)
- Mark Hodges
(California Institute of Technology
California Institute of Technology)
- James Lamb
(California Institute of Technology
California Institute of Technology)
- Paul Rasmussen
(California Institute of Technology
California Institute of Technology)
- Jean Somalwar
(California Institute of Technology)
- Sander Weinreb
(California Institute of Technology)
- David Woody
(California Institute of Technology
California Institute of Technology)
- Joel Leja
(The Pennsylvania State University
The Pennsylvania State University
The Pennsylvania State University)
- Shreya Anand
(California Institute of Technology)
- Kaustav Kashyap Das
(California Institute of Technology)
- Yu-Jing Qin
(California Institute of Technology)
- Sam Rose
(California Institute of Technology)
- Dillon Z. Dong
(California Institute of Technology
National Radio Astronomy Observatory)
- Jessie Miller
(California Institute of Technology)
- Yuhan Yao
(California Institute of Technology
University of California)
Abstract
Fast radio bursts (FRBs) are millisecond-duration events detected from beyond the Milky Way. FRB emission characteristics favour highly magnetized neutron stars, or magnetars, as the sources1, as evidenced by FRB-like bursts from a galactic magnetar2,3, and the star-forming nature of FRB host galaxies4,5. However, the processes that produce FRB sources remain unknown6. Although galactic magnetars are often linked to core-collapse supernovae (CCSNe)7, it is uncertain what determines which supernovae result in magnetars. The galactic environments of FRB sources can be used to investigate their progenitors. Here, we present the stellar population properties of 30 FRB host galaxies discovered by the Deep Synoptic Array (DSA-110). Our analysis shows a marked deficit of low-mass FRB hosts compared with the occurrence of star formation in the Universe, implying that FRBs are a biased tracer of star formation, preferentially selecting massive star-forming galaxies. This bias may be driven by galaxy metallicity, which is positively correlated with stellar mass8. Metal-rich environments may favour the formation of magnetar progenitors through stellar mergers9,10, as higher-metallicity stars are less compact and more likely to fill their Roche lobes, leading to unstable mass transfer. Although massive stars do not have convective interiors to generate strong magnetic fields by dynamo11, merger remnants are thought to have the requisite internal magnetic-field strengths to result in magnetars11,12. The preferential occurrence of FRBs in massive star-forming galaxies suggests that a core-collapse supernova of merger remnants preferentially forms magnetars.
Suggested Citation
Kritti Sharma & Vikram Ravi & Liam Connor & Casey Law & Stella Koch Ocker & Myles Sherman & Nikita Kosogorov & Jakob Faber & Gregg Hallinan & Charlie Harnach & Greg Hellbourg & Rick Hobbs & David Hodg, 2024.
"Preferential occurrence of fast radio bursts in massive star-forming galaxies,"
Nature, Nature, vol. 635(8037), pages 61-66, November.
Handle:
RePEc:nat:nature:v:635:y:2024:i:8037:d:10.1038_s41586-024-08074-9
DOI: 10.1038/s41586-024-08074-9
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