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dc.contributor.authorGunár, Stanislav
dc.contributor.authorHeinzel, Petr
dc.contributor.authorAnzer, Ulrich
dc.contributor.authorMackay, Duncan Hendry
dc.date.accessioned2018-01-22T12:30:05Z
dc.date.available2018-01-22T12:30:05Z
dc.date.issued2018-01-20
dc.identifier.citationGunár , S , Heinzel , P , Anzer , U & Mackay , D H 2018 , ' Quiescent prominences in the era of ALMA. II. Kinetic temperature diagnostics ' , Astrophysical Journal , vol. 853 , no. 1 , 21 . https://doi.org/10.3847/1538-4357/aaa001en
dc.identifier.issn0004-637X
dc.identifier.otherPURE: 251697190
dc.identifier.otherPURE UUID: d9f64642-22fb-4cad-b6a6-42385ea798a4
dc.identifier.otherScopus: 85041109854
dc.identifier.otherORCID: /0000-0001-6065-8531/work/58055459
dc.identifier.otherWOS: 000423090600007
dc.identifier.urihttps://hdl.handle.net/10023/12557
dc.descriptionFunding: UK STFC, the Leverhulme Trust, and NASA (D.H.M.)en
dc.description.abstractWe provide the theoretical background for diagnostics of the thermal properties of solar prominences observed by the Atacama Large Millimeter/submillimeter Array (ALMA). To do this, we employ the 3D Whole-Prominence Fine Structure (WPFS) model that produces synthetic ALMA-like observations of a complex simulated prominence. We use synthetic observations derived at two different submillimeter/millimeter (SMM) wavelengths—one at a wavelength at which the simulated prominence is completely optically thin and another at a wavelength at which a significant portion of the simulated prominence is optically thick—as if these were the actual ALMA observations. This allows us to develop a technique for an analysis of the prominence plasma thermal properties from such a pair of simultaneous high-resolution ALMA observations. The 3D WPFS model also provides detailed information about the distribution of the kinetic temperature and the optical thickness along any line of sight. We can thus assess whether the measure of the kinetic temperature derived from observations accurately represents the actual kinetic temperature properties of the observed plasma. We demonstrate here that in a given pixel the optical thickness at the wavelength at which the prominence plasma is optically thick needs to be above unity or even larger to achieve a sufficient accuracy of the derived information about the kinetic temperature of the analyzed plasma. Information about the optical thickness cannot be directly discerned from observations at the SMM wavelengths alone. However, we show that a criterion that can identify those pixels in which the derived kinetic temperature values correspond well to the actual thermal properties in which the observed prominence can be established.
dc.format.extent11
dc.language.isoeng
dc.relation.ispartofAstrophysical Journalen
dc.rights© 2018, American Astronomical Society. This work has been made available online in accordance with the publisher’s policies. This is the final published version of the work, which was originally published at https://doi.org/10.3847/1538-4357/aaa001en
dc.subjectSun: filaments, prominencesen
dc.subjectSun: radio radiationen
dc.subjectRadiative transferen
dc.subjectMethods: numericalen
dc.subjectQB Astronomyen
dc.subjectQC Physicsen
dc.subjectNDASen
dc.subject.lccQBen
dc.subject.lccQCen
dc.titleQuiescent prominences in the era of ALMA. II. Kinetic temperature diagnosticsen
dc.typeJournal articleen
dc.contributor.sponsorScience & Technology Facilities Councilen
dc.contributor.sponsorScience & Technology Facilities Councilen
dc.contributor.sponsorThe Royal Society of Edinburghen
dc.description.versionPublisher PDFen
dc.contributor.institutionUniversity of St Andrews. Applied Mathematicsen
dc.identifier.doihttps://doi.org/10.3847/1538-4357/aaa001
dc.description.statusPeer revieweden
dc.date.embargoedUntil2018-01-18
dc.identifier.grantnumberST/N000609/1en
dc.identifier.grantnumberST/K000950/1en
dc.identifier.grantnumberN/Aen


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