<p>Fast radio bursts (FRBs) last for milliseconds and arrive at Earth from cosmological distances. Although their origins and emission mechanisms are unknown, their signals bear similarities with the much less luminous radio emission generated by pulsars within our Miky Way Galaxy<sup><CitationRef CitationID="CR1">1</CitationRef></sup>, with properties suggesting neutron star origins<sup><CitationRef CitationID="CR2">2</CitationRef>,<CitationRef CitationID="CR3">3</CitationRef></sup>. However, unlike pulsars, FRBs typically show minimal variability in their linear polarization position angle (PA) curves<sup><CitationRef CitationID="CR4">4</CitationRef></sup>. Even when marked PA evolution is present, their curves deviate significantly from the canonical shape predicted by the rotating vector model (RVM) of pulsars<sup><CitationRef CitationID="CR5">5</CitationRef></sup>. Here we report on FRB 20221022A, detected by the Canadian Hydrogen Intensity Mapping Experiment Fast Radio Burst project (CHIME/FRB) and localized to a nearby host galaxy (about 65 Mpc), MCG+14-02-011. This FRB shows a notable approximately 130° PA rotation over its about 2.5 ms burst duration, resembling the characteristic S-shaped evolution seen in many pulsars and some radio magnetars. The observed PA evolution supports magnetospheric origins<sup><CitationRef AdditionalCitationIDS="CR7" CitationID="CR6">6</CitationRef>–<CitationRef CitationID="CR8">8</CitationRef></sup> over models involving distant shocks<sup><CitationRef AdditionalCitationIDS="CR10" CitationID="CR9">9</CitationRef>–<CitationRef CitationID="CR11">11</CitationRef></sup>, echoing similar conclusions drawn from tempo-polarimetric studies of some repeating FRBs<sup><CitationRef CitationID="CR12">12</CitationRef>,<CitationRef CitationID="CR13">13</CitationRef></sup>. The PA evolution is well described by the RVM and, although we cannot determine the inclination and magnetic obliquity because of the unknown period or duty cycle of the source, we exclude very short-period pulsars (for example, recycled millisecond pulsars) as the progenitor.</p>

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A pulsar-like polarization angle swing from a nearby fast radio burst

  • Ryan Mckinven,
  • Mohit Bhardwaj,
  • Tarraneh Eftekhari,
  • Charles D. Kilpatrick,
  • Aida Kirichenko,
  • Arpan Pal,
  • Amanda M. Cook,
  • B. M. Gaensler,
  • Utkarsh Giri,
  • Victoria M. Kaspi,
  • Daniele Michilli,
  • Kenzie Nimmo,
  • Aaron B. Pearlman,
  • Ziggy Pleunis,
  • Ketan R. Sand,
  • Ingrid Stairs,
  • Bridget C. Andersen,
  • Shion Andrew,
  • Kevin Bandura,
  • Charanjot Brar,
  • Tomas Cassanelli,
  • Shami Chatterjee,
  • Alice P. Curtin,
  • Fengqiu Adam Dong,
  • Gwendolyn Eadie,
  • Emmanuel Fonseca,
  • Adaeze L. Ibik,
  • Jane F. Kaczmarek,
  • Bikash Kharel,
  • Mattias Lazda,
  • Calvin Leung,
  • Dongzi Li,
  • Robert Main,
  • Kiyoshi W. Masui,
  • Juan Mena-Parra,
  • Cherry Ng,
  • Ayush Pandhi,
  • Swarali Shivraj Patil,
  • J. Xavier Prochaska,
  • Masoud Rafiei-Ravandi,
  • Paul Scholz,
  • Vishwangi Shah,
  • Kaitlyn Shin,
  • Kendrick Smith

摘要

Fast radio bursts (FRBs) last for milliseconds and arrive at Earth from cosmological distances. Although their origins and emission mechanisms are unknown, their signals bear similarities with the much less luminous radio emission generated by pulsars within our Miky Way Galaxy1, with properties suggesting neutron star origins2,3. However, unlike pulsars, FRBs typically show minimal variability in their linear polarization position angle (PA) curves4. Even when marked PA evolution is present, their curves deviate significantly from the canonical shape predicted by the rotating vector model (RVM) of pulsars5. Here we report on FRB 20221022A, detected by the Canadian Hydrogen Intensity Mapping Experiment Fast Radio Burst project (CHIME/FRB) and localized to a nearby host galaxy (about 65 Mpc), MCG+14-02-011. This FRB shows a notable approximately 130° PA rotation over its about 2.5 ms burst duration, resembling the characteristic S-shaped evolution seen in many pulsars and some radio magnetars. The observed PA evolution supports magnetospheric origins68 over models involving distant shocks911, echoing similar conclusions drawn from tempo-polarimetric studies of some repeating FRBs12,13. The PA evolution is well described by the RVM and, although we cannot determine the inclination and magnetic obliquity because of the unknown period or duty cycle of the source, we exclude very short-period pulsars (for example, recycled millisecond pulsars) as the progenitor.