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dc.contributor.authorPunanova, A.en
dc.contributor.authorVasyunin, A.en
dc.contributor.authorCaselli, P.en
dc.contributor.authorHoward, A.en
dc.contributor.authorSpezzano, S.en
dc.contributor.authorShirley, Y.en
dc.contributor.authorScibelli, S.en
dc.contributor.authorHarju, J.en
dc.date.accessioned2022-10-19T05:24:26Z-
dc.date.available2022-10-19T05:24:26Z-
dc.date.issued2022-
dc.identifier.citationMethanol Mapping in Cold Cores: Testing Model Predictions / A. Punanova, A. Vasyunin, P. Caselli et al. // Astrophysical Journal. — 2022. — Vol. 927. — Iss. 2. — 213.en
dc.identifier.issn0004637X-
dc.identifier.otherhttps://www.scopus.com/inward/record.uri?eid=2-s2.0-85127313812&doi=10.3847%2f1538-4357%2fac4e7d&partnerID=40&md5=72f0e44020e578aaeb8cdaf68abdedaclink
dc.identifier.urihttp://elar.urfu.ru/handle/10995/118315-
dc.description.abstractChemical models predict that in cold cores gas-phase methanol is expected to be abundant at the outer edge of the CO depletion zone, where CO is actively adsorbed. CO adsorption correlates with volume density in cold cores, and, in nearby molecular clouds, catastrophic CO freeze-out happens at volume densities above 104 cm-3. The methanol production rate is maximized there and its freeze-out rate does not overcome its production rate, while the molecules are shielded from UV destruction by gas and dust. Thus, in cold cores, methanol abundance should generally correlate with visual extinction, which depends on both volume and column density. In this work, we test the most basic model prediction that maximum methanol abundance is associated with a local A V ∼4 mag in dense cores and constrain the model parameters with the observational data. With the IRAM 30 m antenna, we mapped the CH3OH (2-1) and (3-2) transitions toward seven dense cores in the L1495 filament in Taurus to measure the methanol abundance. We use the Herschel/SPIRE maps to estimate visual extinction, and the C18O(2-1) maps from Tafalla & Hacar to estimate CO depletion. We explored the observed and modeled correlations between the methanol abundances, CO depletion, and visual extinction, varying the key model parameters. The modeling results show that hydrogen surface diffusion via tunneling is crucial to reproduce the observed methanol abundances, and the necessary reactive desorption efficiency matches the one deduced from laboratory experiments. © 2022. The Author(s). Published by the American Astronomical Society.en
dc.description.sponsorshipDGE-1143953; National Science Foundation, NSF; Ministry of Education and Science of the Russian Federation, Minobrnauka: FEUZ-2020-0038; Centre National de la Recherche Scientifique, CNRS; Russian Science Foundation, RSF: 18-12-00351en
dc.description.sponsorshipThis work is based on observations carried out under projects 013-18, 125-18, and 031-19 with the IRAM 30 m telescope. Institut de Radioastronomie Millimétrique (IRAM) is supported by INSU/CNRS (France), MPG (Germany), and IGN (Spain).en
dc.description.sponsorshipThe authors thank the anonymous referee for valuable comments that helped to improve the manuscript. A.V. and A.P. are members of the Max Planck Partner Group at the Ural Federal University. A.P. and A.V. acknowledge the support of the Russian Science Foundation project 18-12-00351 and of the Russian Ministry of Science and Education via the State Assignment Contract no. FEUZ-2020-0038 (discussion on elemental abundances). The authors thank Vadim Krushinskiy for his help with Matplotlib and Gleb Fedoseev for discussion about photodesorption yield. S.S. is supported by National Science Foundation Graduate Research Fellowship (NSF GRF) Grant DGE-1143953.en
dc.format.mimetypeapplication/pdfen
dc.language.isoenen
dc.publisherIOP Publishing Ltden
dc.relationinfo:eu-repo/grantAgreement/RSF//18-12-00351en
dc.rightsinfo:eu-repo/semantics/openAccessen
dc.sourceAstrophysical Journalen
dc.titleMethanol Mapping in Cold Cores: Testing Model Predictionsen
dc.typeArticleen
dc.typeinfo:eu-repo/semantics/articleen
dc.typeinfo:eu-repo/semantics/publishedVersionen
dc.identifier.doi10.3847/1538-4357/ac4e7d-
dc.identifier.scopus85127313812-
local.contributor.employeePunanova, A., Ural Federal University, 19 Mira street, Yekaterinburg, 620002, Russian Federationen
local.contributor.employeeVasyunin, A., Ural Federal University, 19 Mira street, Yekaterinburg, 620002, Russian Federationen
local.contributor.employeeCaselli, P., Max-Planck-Institut für Extraterrestrische Physik, Giessenbachstrasse 1, Garching, D-85748, Germanyen
local.contributor.employeeHoward, A., School of Physics and Astronomy, Cardiff University, 5 The Parade, Cardiff, CF24 3AA, United Kingdomen
local.contributor.employeeSpezzano, S., Max-Planck-Institut für Extraterrestrische Physik, Giessenbachstrasse 1, Garching, D-85748, Germanyen
local.contributor.employeeShirley, Y., Steward Observatory, University of Arizona, Tucson, AZ 85721, United Statesen
local.contributor.employeeScibelli, S., Steward Observatory, University of Arizona, Tucson, AZ 85721, United Statesen
local.contributor.employeeHarju, J., Max-Planck-Institut für Extraterrestrische Physik, Giessenbachstrasse 1, Garching, D-85748, Germany, Department of Physics, University of Helsinki, P.O. Box 64FI-00014, Finlanden
local.issue2-
local.volume927-
dc.identifier.wos000770130600001-
local.contributor.departmentUral Federal University, 19 Mira street, Yekaterinburg, 620002, Russian Federationen
local.contributor.departmentMax-Planck-Institut für Extraterrestrische Physik, Giessenbachstrasse 1, Garching, D-85748, Germanyen
local.contributor.departmentSchool of Physics and Astronomy, Cardiff University, 5 The Parade, Cardiff, CF24 3AA, United Kingdomen
local.contributor.departmentSteward Observatory, University of Arizona, Tucson, AZ 85721, United Statesen
local.contributor.departmentDepartment of Physics, University of Helsinki, P.O. Box 64FI-00014, Finlanden
local.identifier.pure29926789-
local.description.order213-
local.identifier.eid2-s2.0-85127313812-
local.fund.rsf18-12-00351-
local.identifier.wosWOS:000770130600001-
local.fund.feuzFEUZ-2020-0038-
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