The Nature of γ-Ray Emission from HESS J1912+101

Since the discovery of HESS J1912+101 at teraelectronvolt energies, its nature has been extensively studied. Due to the absence of X-ray and radio counterparts, whether its γ -ray emission is produced by relativistic electrons or ions is still a matter of debate. We reanalyze its megaelectronvolt to...

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Published in:The Astrophysical Journal
Main Authors: Yuan Li, Siming Liu, Yu He
Format: Article
Language:English
Published: IOP Publishing 2023-01-01
Subjects:
Online Access:https://doi.org/10.3847/1538-4357/ace344
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author Yuan Li
Siming Liu
Yu He
author_facet Yuan Li
Siming Liu
Yu He
author_sort Yuan Li
collection DOAJ
container_title The Astrophysical Journal
description Since the discovery of HESS J1912+101 at teraelectronvolt energies, its nature has been extensively studied. Due to the absence of X-ray and radio counterparts, whether its γ -ray emission is produced by relativistic electrons or ions is still a matter of debate. We reanalyze its megaelectronvolt to gigaelectronvolt γ -ray emission using 14 yr of Pass 8 data of the Fermi-LAT, and find that the gigaelectronvolt γ -ray emission is more extended than the teraelectronvolt shell detected by H. E. S. S. and flux above 10 GeV from the northern half is much higher than that from the southern half, where there is evident interaction between shocks and molecular clouds. As a consequence, the gigaelectronvolt spectrum of the northern half (with an index of 2.19 ± 0.12) is much harder than that in the south (with an index of 2.72 ± 0.08), and the overall gigaelectronvolt spectrum shows a concave shape, which is distinct from most γ -ray supernova remnants (SNRs). In combination with the teraelectronvolt spectrum, the overall γ -ray spectrum can be fitted with a broken power-law model for trapped ions and a low energy component due to escaping ions. The diffusion coefficient for escaping ions however needs to be proportional to the energy, implying that the low energy component may also be attributed to ions accelerated via recent shock–cloud interactions. A hadronic origin for the γ -ray emission is therefore favored and the overall emission properties are consistent with ion acceleration by SNR shocks. On the other hand, it is still undeniable that stellar cluster or PWN may have some contribution in some parts of this extended source.
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spelling doaj-art-e3918c8f8d2f41ccbce31e14b40dfd492025-08-19T22:22:11ZengIOP PublishingThe Astrophysical Journal1538-43572023-01-01953110010.3847/1538-4357/ace344The Nature of γ-Ray Emission from HESS J1912+101Yuan Li0https://orcid.org/0009-0003-4873-6770Siming Liu1https://orcid.org/0000-0003-1039-9521Yu He2https://orcid.org/0000-0002-2745-9001School of Physical Science and Technology, Southwest Jiaotong University , Chengdu 610031, People’s Republic of China ; liusm@swjtu.edu.cn, heyujy@swjtu.edu.cn; Tsung-Dao Lee Institute, Shanghai Jiao Tong University , Shanghai 200240, People’s Republic of China; School of Physics and Astronomy, Shanghai Jiao Tong University , Shanghai 200240, People’s Republic of ChinaSchool of Physical Science and Technology, Southwest Jiaotong University , Chengdu 610031, People’s Republic of China ; liusm@swjtu.edu.cn, heyujy@swjtu.edu.cnSchool of Physical Science and Technology, Southwest Jiaotong University , Chengdu 610031, People’s Republic of China ; liusm@swjtu.edu.cn, heyujy@swjtu.edu.cnSince the discovery of HESS J1912+101 at teraelectronvolt energies, its nature has been extensively studied. Due to the absence of X-ray and radio counterparts, whether its γ -ray emission is produced by relativistic electrons or ions is still a matter of debate. We reanalyze its megaelectronvolt to gigaelectronvolt γ -ray emission using 14 yr of Pass 8 data of the Fermi-LAT, and find that the gigaelectronvolt γ -ray emission is more extended than the teraelectronvolt shell detected by H. E. S. S. and flux above 10 GeV from the northern half is much higher than that from the southern half, where there is evident interaction between shocks and molecular clouds. As a consequence, the gigaelectronvolt spectrum of the northern half (with an index of 2.19 ± 0.12) is much harder than that in the south (with an index of 2.72 ± 0.08), and the overall gigaelectronvolt spectrum shows a concave shape, which is distinct from most γ -ray supernova remnants (SNRs). In combination with the teraelectronvolt spectrum, the overall γ -ray spectrum can be fitted with a broken power-law model for trapped ions and a low energy component due to escaping ions. The diffusion coefficient for escaping ions however needs to be proportional to the energy, implying that the low energy component may also be attributed to ions accelerated via recent shock–cloud interactions. A hadronic origin for the γ -ray emission is therefore favored and the overall emission properties are consistent with ion acceleration by SNR shocks. On the other hand, it is still undeniable that stellar cluster or PWN may have some contribution in some parts of this extended source.https://doi.org/10.3847/1538-4357/ace344Supernova remnantsMolecular cloudsHigh energy astrophysics
spellingShingle Yuan Li
Siming Liu
Yu He
The Nature of γ-Ray Emission from HESS J1912+101
Supernova remnants
Molecular clouds
High energy astrophysics
title The Nature of γ-Ray Emission from HESS J1912+101
title_full The Nature of γ-Ray Emission from HESS J1912+101
title_fullStr The Nature of γ-Ray Emission from HESS J1912+101
title_full_unstemmed The Nature of γ-Ray Emission from HESS J1912+101
title_short The Nature of γ-Ray Emission from HESS J1912+101
title_sort nature of γ ray emission from hess j1912 101
topic Supernova remnants
Molecular clouds
High energy astrophysics
url https://doi.org/10.3847/1538-4357/ace344
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