Identifying the counterpart of HESS J1858+020

Aims: HESS J1858+020 is a weak γ-ray source that does not have any clear cataloged counterpart at any wavelengths. Recently, the source G35.6-0.4 was re-identified as a SNR. The HESS source lies towards the southern border of this remnant. The purpose of this work is to investigate the interstellar...

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Autores principales: Paron, S., Giacani, E.
Formato: JOUR
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ISM
Acceso en línea:http://hdl.handle.net/20.500.12110/paper_00046361_v509_n1_p_Paron
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spelling todo:paper_00046361_v509_n1_p_Paron2023-10-03T14:00:30Z Identifying the counterpart of HESS J1858+020 Paron, S. Giacani, E. Clouds - ISM Individual objects ISM ISM - ISM Supernova remnants - Gamma rays Clouds Elementary particles Signal to noise ratio Stars Clouds-ISM Individual objects ISM ISM - ISM Supernova remnants Gamma rays Aims: HESS J1858+020 is a weak γ-ray source that does not have any clear cataloged counterpart at any wavelengths. Recently, the source G35.6-0.4 was re-identified as a SNR. The HESS source lies towards the southern border of this remnant. The purpose of this work is to investigate the interstellar medium around the mentioned sources to look for possible counterparts of the very high energy emission. Methods: Using the 13CO J = 1-0 line from the Galactic Ring Survey and mid-IR data from GLIMPSE we analyze the environs of HESS J1858+020 and SNR G35.6-0.4. Results. The 13CO data show the presence of a molecular cloud towards the southern border of SNR G35.6-0.4 and at the same distance as the remnant. This cloud is composed of two molecular clumps, one over the SNR shell and the other located at the center of HESS J1858+020. We estimate a molecular mass and a density of ∼5 × 103 M⊙ and ∼500 cm -3 respectively for each clump. Considering the gamma-ray flux observed towards HESS J1858+020, we estimate that a molecular cloud with a density of at least 150 cm-3 could explain the very high energy emission hadronically. Thus, we suggest that the γ-ray emission detected in HESS J1858+020 is due to hadronic mechanism. Additionally, analyzing mid-IR emission, we find that the region is active in star formation, which could be considered as an alternative or complementary possibility to explain the very high energy emission. © ESO 2010. JOUR info:eu-repo/semantics/openAccess http://creativecommons.org/licenses/by/2.5/ar http://hdl.handle.net/20.500.12110/paper_00046361_v509_n1_p_Paron
institution Universidad de Buenos Aires
institution_str I-28
repository_str R-134
collection Biblioteca Digital - Facultad de Ciencias Exactas y Naturales (UBA)
topic Clouds - ISM
Individual objects
ISM
ISM - ISM
Supernova remnants - Gamma rays
Clouds
Elementary particles
Signal to noise ratio
Stars
Clouds-ISM
Individual objects
ISM
ISM - ISM
Supernova remnants
Gamma rays
spellingShingle Clouds - ISM
Individual objects
ISM
ISM - ISM
Supernova remnants - Gamma rays
Clouds
Elementary particles
Signal to noise ratio
Stars
Clouds-ISM
Individual objects
ISM
ISM - ISM
Supernova remnants
Gamma rays
Paron, S.
Giacani, E.
Identifying the counterpart of HESS J1858+020
topic_facet Clouds - ISM
Individual objects
ISM
ISM - ISM
Supernova remnants - Gamma rays
Clouds
Elementary particles
Signal to noise ratio
Stars
Clouds-ISM
Individual objects
ISM
ISM - ISM
Supernova remnants
Gamma rays
description Aims: HESS J1858+020 is a weak γ-ray source that does not have any clear cataloged counterpart at any wavelengths. Recently, the source G35.6-0.4 was re-identified as a SNR. The HESS source lies towards the southern border of this remnant. The purpose of this work is to investigate the interstellar medium around the mentioned sources to look for possible counterparts of the very high energy emission. Methods: Using the 13CO J = 1-0 line from the Galactic Ring Survey and mid-IR data from GLIMPSE we analyze the environs of HESS J1858+020 and SNR G35.6-0.4. Results. The 13CO data show the presence of a molecular cloud towards the southern border of SNR G35.6-0.4 and at the same distance as the remnant. This cloud is composed of two molecular clumps, one over the SNR shell and the other located at the center of HESS J1858+020. We estimate a molecular mass and a density of ∼5 × 103 M⊙ and ∼500 cm -3 respectively for each clump. Considering the gamma-ray flux observed towards HESS J1858+020, we estimate that a molecular cloud with a density of at least 150 cm-3 could explain the very high energy emission hadronically. Thus, we suggest that the γ-ray emission detected in HESS J1858+020 is due to hadronic mechanism. Additionally, analyzing mid-IR emission, we find that the region is active in star formation, which could be considered as an alternative or complementary possibility to explain the very high energy emission. © ESO 2010.
format JOUR
author Paron, S.
Giacani, E.
author_facet Paron, S.
Giacani, E.
author_sort Paron, S.
title Identifying the counterpart of HESS J1858+020
title_short Identifying the counterpart of HESS J1858+020
title_full Identifying the counterpart of HESS J1858+020
title_fullStr Identifying the counterpart of HESS J1858+020
title_full_unstemmed Identifying the counterpart of HESS J1858+020
title_sort identifying the counterpart of hess j1858+020
url http://hdl.handle.net/20.500.12110/paper_00046361_v509_n1_p_Paron
work_keys_str_mv AT parons identifyingthecounterpartofhessj1858020
AT giacanie identifyingthecounterpartofhessj1858020
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