Striped Jets in Post–Neutron Star Merger Systems

Models invoking magnetic reconnection as the particle acceleration mechanism within relativistic jets often adopt a gradual energy dissipation profile within the jet. However, such a profile has yet to be reproduced in first-principles simulations. Here we perform a suite of 3D general relativistic...

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Main Authors: Emma Kaufman, I. M. Christie, A. Lalakos, A. Tchekhovskoy, D. Giannios
Format: Article
Language:English
Published: IOP Publishing 2023-01-01
Series:The Astrophysical Journal
Subjects:
Online Access:https://doi.org/10.3847/1538-4357/ace894
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author Emma Kaufman
I. M. Christie
A. Lalakos
A. Tchekhovskoy
D. Giannios
author_facet Emma Kaufman
I. M. Christie
A. Lalakos
A. Tchekhovskoy
D. Giannios
author_sort Emma Kaufman
collection DOAJ
description Models invoking magnetic reconnection as the particle acceleration mechanism within relativistic jets often adopt a gradual energy dissipation profile within the jet. However, such a profile has yet to be reproduced in first-principles simulations. Here we perform a suite of 3D general relativistic magnetohydrodynamic simulations of post–neutron star merger disks with an initially purely toroidal magnetic field. We explore the variations in both the microphysics (e.g., nuclear recombination, neutrino emission) and system parameters (e.g, disk mass). In all of our simulations, we find the formation of magnetically striped jets. The stripes result from the reversals in the poloidal magnetic flux polarity generated in the accretion disk. The simulations display large variations in the distributions of stripe duration, τ , and power, 〈 P _Φ 〉. We find that more massive disks produce more powerful stripes, the most powerful of which reaches 〈 P _Φ 〉 ∼ 10 ^49 erg s ^−1 at τ ∼ 20 ms. The power and variability that result from the magnetic reconnection of the stripes agree with those inferred in short-duration gamma-ray bursts. We find that the dissipation profile of the cumulative energy is roughly a power law in both radial distance, z , and τ , with a slope in the range of ∼1.7–3; more massive disks display larger slopes.
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spelling doaj.art-6072ce921dfa4e8ebd102c052c526c552023-09-03T15:13:20ZengIOP PublishingThe Astrophysical Journal1538-43572023-01-0195414010.3847/1538-4357/ace894Striped Jets in Post–Neutron Star Merger SystemsEmma Kaufman0https://orcid.org/0000-0002-7236-284XI. M. Christie1A. Lalakos2https://orcid.org/0000-0002-6883-6520A. Tchekhovskoy3D. Giannios4Center for Interdisciplinary Exploration & Research in Astrophysics (CIERA), Physics & Astronomy, Northwestern University , Evanston, IL 60208, USA ekaufman@u.northwestern.edu, ichristi231@gmail.comCenter for Interdisciplinary Exploration & Research in Astrophysics (CIERA), Physics & Astronomy, Northwestern University , Evanston, IL 60208, USA ekaufman@u.northwestern.edu, ichristi231@gmail.comCenter for Interdisciplinary Exploration & Research in Astrophysics (CIERA), Physics & Astronomy, Northwestern University , Evanston, IL 60208, USA ekaufman@u.northwestern.edu, ichristi231@gmail.comCenter for Interdisciplinary Exploration & Research in Astrophysics (CIERA), Physics & Astronomy, Northwestern University , Evanston, IL 60208, USA ekaufman@u.northwestern.edu, ichristi231@gmail.comDepartment of Physics and Astronomy, Purdue University , 525 Northwestern Avenue, West Lafayette, IN 47907, USAModels invoking magnetic reconnection as the particle acceleration mechanism within relativistic jets often adopt a gradual energy dissipation profile within the jet. However, such a profile has yet to be reproduced in first-principles simulations. Here we perform a suite of 3D general relativistic magnetohydrodynamic simulations of post–neutron star merger disks with an initially purely toroidal magnetic field. We explore the variations in both the microphysics (e.g., nuclear recombination, neutrino emission) and system parameters (e.g, disk mass). In all of our simulations, we find the formation of magnetically striped jets. The stripes result from the reversals in the poloidal magnetic flux polarity generated in the accretion disk. The simulations display large variations in the distributions of stripe duration, τ , and power, 〈 P _Φ 〉. We find that more massive disks produce more powerful stripes, the most powerful of which reaches 〈 P _Φ 〉 ∼ 10 ^49 erg s ^−1 at τ ∼ 20 ms. The power and variability that result from the magnetic reconnection of the stripes agree with those inferred in short-duration gamma-ray bursts. We find that the dissipation profile of the cumulative energy is roughly a power law in both radial distance, z , and τ , with a slope in the range of ∼1.7–3; more massive disks display larger slopes.https://doi.org/10.3847/1538-4357/ace894JetsGamma-ray burstsMagnetohydrodynamical simulations
spellingShingle Emma Kaufman
I. M. Christie
A. Lalakos
A. Tchekhovskoy
D. Giannios
Striped Jets in Post–Neutron Star Merger Systems
The Astrophysical Journal
Jets
Gamma-ray bursts
Magnetohydrodynamical simulations
title Striped Jets in Post–Neutron Star Merger Systems
title_full Striped Jets in Post–Neutron Star Merger Systems
title_fullStr Striped Jets in Post–Neutron Star Merger Systems
title_full_unstemmed Striped Jets in Post–Neutron Star Merger Systems
title_short Striped Jets in Post–Neutron Star Merger Systems
title_sort striped jets in post neutron star merger systems
topic Jets
Gamma-ray bursts
Magnetohydrodynamical simulations
url https://doi.org/10.3847/1538-4357/ace894
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AT atchekhovskoy stripedjetsinpostneutronstarmergersystems
AT dgiannios stripedjetsinpostneutronstarmergersystems