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Authordc.contributor.authorRiquelme, D. 
Authordc.contributor.authorAmo Baladrón, M. A. 
Authordc.contributor.authorMartín-Pintado, J. 
Authordc.contributor.authorMauersberger, R. 
Authordc.contributor.authorMartin, S. 
Authordc.contributor.authorBurton, M. G. 
Authordc.contributor.authorCunningham, M. 
Authordc.contributor.authorJones, P. A. 
Authordc.contributor.authorMenten, K. M. 
Authordc.contributor.authorBronfman Aguiló, Leonardo 
Authordc.contributor.authorGuesten, R. 
Admission datedc.date.accessioned2018-10-08T14:08:11Z
Available datedc.date.available2018-10-08T14:08:11Z
Publication datedc.date.issued2018-05-30
Cita de ítemdc.identifier.citationA&A 613, A42 (2018)es_ES
Identifierdc.identifier.other10.1051/0004-6361/201629065
Identifierdc.identifier.urihttps://repositorio.uchile.cl/handle/2250/151993
Abstractdc.description.abstractAims. We aim to reveal the morphology, chemical composition, kinematics, and to establish the main processes prevalent in the gas at the footpoints of the giant molecular loops (GMLs) in the Galactic center region. Methods. Using the 22-m Mopra telescope, we mapped the M-3.8+0.9 molecular cloud, placed at the footpoints of a GML, in 3 -mm range molecular lines. To derive the molecular hydrogen column density, we also observed the (13)C0(2 1) line at 1 mm using the 12-m APEX telescope. From the 3 mm observations 12 molecular species were detected, namely HCO, HCN, (HCN)-C-13, HNC, SiO, CS, CH3OH, N2H+, SO, HNCO, OCS, and HC3N. Results. Maps revealing the morphology and kinematics of the M-3.8+0.9 molecular cloud in different molecules are presented. We identify six main molecular complexes. We derive fractional abundances in 11 selected positions of the different molecules assuming local thermodynamical equilibrium. Conclusions. Most of the fractional abundances derived for the M-3.8+0.9 molecular cloud are very similar over the whole cloud. However, the fractional abundances of some molecules show significant difference with respect to those measured in the central molecular zone (CMZ). The abundances of the shock tracer SiO are very similar between the GMLs and the CMZ. The methanol emission is the most abundant species in the GMLs. This indicates that the gas is likely affected by moderate similar to 30 km s(-1) or even high velocity (50 km s(-1)) shocks, consistent with the line profile observed toward one of the studied position. The origin of the shocks is likely related to the flow of the gas throughout the GMLs towards the footpoints.es_ES
Patrocinadordc.description.sponsorshipDeutsche Forschungsgemeinschaft (DFG) DGI AYA 2008-06181-C02-02 CONICYT PFB-06 MINECO AYA2010-2169-C04-01 FIS2012-39162-C06-01 ESP2013-47809-C03-01 ESP2015-65597-C4-1 Australian Government Australian Research Counciles_ES
Lenguagedc.language.isoenes_ES
Publisherdc.publisherEDP Scienceses_ES
Type of licensedc.rightsAttribution-NonCommercial-NoDerivs 3.0 Chile*
Link to Licensedc.rights.urihttp://creativecommons.org/licenses/by-nc-nd/3.0/cl/*
Sourcedc.sourceAstronomy & Astrophysicses_ES
Keywordsdc.subjectISM: moleculeses_ES
Keywordsdc.subjectGalaxy: centeres_ES
Keywordsdc.subjectISM: cloudses_ES
Títulodc.titleFootpoints of the giant molecular loops in the galactic center regiones_ES
Document typedc.typeArtículo de revista
Catalogueruchile.catalogadorrgfes_ES
Indexationuchile.indexArtículo de publicación ISIes_ES


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Attribution-NonCommercial-NoDerivs 3.0 Chile
Except where otherwise noted, this item's license is described as Attribution-NonCommercial-NoDerivs 3.0 Chile