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xmlns:vodm="http://www.ivoa.net/xml/DataModel/v1" xmlns:voe="http://www.ivoa.net/xml/VOEventRegExt/v2" xmlns:vosi10="http://www.ivoa.net/xml/VOSITables/v1.0" xmlns:vot="http://www.ivoa.net/xml/VOTable/v1.2" xmlns:vot0="http://www.ivoa.net/xml/VOTable/v1.3" xmlns:vot1="http://www.ivoa.net/xml/VOTable/v1.1" xmlns:vr="http://www.ivoa.net/xml/VOResource/v1.0" xmlns:vr0="https://www.ivoa.net/xml/VOResource/v1.0" xmlns:vr1="http://www.ivoa.net/xml/VOResource/v1.1" xmlns:vr2="http://Www.ivoa.net/xml/VOResource/v1.0" xmlns:vr3="http://www.ivoa.net/xml/VOResource/v1%20.0" xmlns:vs="http://www.ivoa.net/xml/VODataService/v1.1" xmlns:vs0="http://www.ivoa.net/xml/VODataService/v1.0" xmlns:vs1="https://www.ivoa.net/xml/VODataService/v1.0" xmlns:vstd="http://www.ivoa.net/xml/StandardsRegExt/v1.0" xmlns:xdtn="http://www.w3.org/2004/07/xpath-datatypes" xmlns:xlink="http://www.w3.org/1999/xlink" xmlns:xlink0="https://www.w3.org/1999/xlink" xmlns:xsd="http://www.w3.org/2001/XMLSchema" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xmlns:xsi0="https://www.w3.org/2001/XMLSchema-instance" xmlns:xu="http://www.xmldb.org/xupdate"><oai:identifier>ivo://CDS.VizieR/J/ApJ/856/52</oai:identifier><oai:datestamp>2025-06-13T15:25:00Z</oai:datestamp><oai:setSpec>J.ApJ</oai:setSpec></oai:header><oai:metadata><eudc:resource xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xmlns:eudc="http://schema.eudat.eu/schema/kernel-1" xmlns:ri="http://www.ivoa.net/xml/RegistryInterface/v1.0" xmlns:vr="http://www.ivoa.net/xml/VOResource/v1.0" xmlns:oai="http://www.openarchives.org/OAI/2.0/" xmlns:dachs="urn:dachs" xsi:schemaLocation="http://schema.eudat.eu/schema/kernel-1           http://docs.g-vo.org/schemata/eudat-core.xsd"><eudc:community>IVOA</eudc:community><eudc:titles><eudc:title>Kinematic distances of star-forming regions</eudc:title></eudc:titles><eudc:descriptions><eudc:description>Distances to high-mass star-forming regions (HMSFRs) in the Milky Way are a crucial constraint on the structure of the Galaxy. Only kinematic distances are available for a majority of the HMSFRs in the Milky Way. Here, we compare the kinematic and parallax distances of 75 Galactic HMSFRs to assess the accuracy of kinematic distances. We derive the kinematic distances using three different methods: the traditional method using the Brand &amp; Blitz (1993, J/A+A/275/67) rotation curve (Method A), the traditional method using the Reid+ (2014, J/ApJ/783/130) rotation curve and updated solar motion parameters (Method B), and a Monte Carlo technique (Method C). Methods B and C produce kinematic distances closest to the parallax distances, with median differences of 13% (0.43kpc) and 17% (0.42kpc), respectively. Except in the vicinity of the tangent point, the kinematic distance uncertainties derived by Method C are smaller than those of Methods A and B. In a large region of the Galaxy, the Method C kinematic distances constrain both the distances and the Galactocentric positions of HMSFRs more accurately than parallax distances. Beyond the tangent point along l=30{deg}, for example, the Method C kinematic distance uncertainties reach a minimum of 10% of the parallax distance uncertainty at a distance of 14kpc. We develop a prescription for deriving and applying the Method C kinematic distances and distance uncertainties. The code to generate the Method C kinematic distances is publicly available and may be utilized through an online tool.</eudc:description></eudc:descriptions><eudc:keywords><eudc:keyword>h-ii-regions</eudc:keyword><eudc:keyword>giant-stars</eudc:keyword><eudc:keyword>stellar-distance</eudc:keyword><eudc:keyword>radio-sources</eudc:keyword><eudc:keyword>visible-astronomy</eudc:keyword><eudc:keyword>trigonometric-parallax</eudc:keyword><eudc:keyword>milky-way-galaxy</eudc:keyword><eudc:keyword>star-forming-regions</eudc:keyword><eudc:keyword>galactic-and-extragalactic-astronomy</eudc:keyword><eudc:keyword>stellar-astronomy</eudc:keyword><eudc:keyword>cosmology</eudc:keyword><eudc:keyword>observational-astronomy</eudc:keyword><eudc:keyword>interstellar-medium</eudc:keyword></eudc:keywords><eudc:identifiers><eudc:identifier identifierType="URL">https://dc.g-vo.org/rr/q/lp/custom/CDS.VizieR/J/ApJ/856/52</eudc:identifier><eudc:identifier identifierType="DOI">http://doi.org/10.26093/cds/vizier.18560052</eudc:identifier></eudc:identifiers><eudc:relatedIdentifiers><eudc:relatedIdentifier relatedIdentifierType="URL">https://cdsarc.cds.unistra.fr/viz-bin/cat/J/ApJ/856/52</eudc:relatedIdentifier><eudc:relatedIdentifier relatedIdentifierType="bibcode">2018ApJ...856...52W</eudc:relatedIdentifier><eudc:relatedIdentifier relatedIdentifierType="URL">https://vizier.cds.unistra.fr/viz-bin/VizieR-2?-source=J/ApJ/856/52</eudc:relatedIdentifier><eudc:description>Cone search capability for table J/ApJ/856/52/sample (High-mass star-forming region (including 3 red supergiants) (Table 1) and Monte Carlo parallax and derived kinematic distances (Table 3))</eudc:description></eudc:relatedIdentifiers><eudc:creators><eudc:creator><eudc:creatorName>Wenger T.V.</eudc:creatorName></eudc:creator><eudc:creator><eudc:creatorName>Balser D.S.</eudc:creatorName></eudc:creator><eudc:creator><eudc:creatorName>Anderson L.D.</eudc:creatorName></eudc:creator><eudc:creator><eudc:creatorName>Bania T.M.</eudc:creatorName></eudc:creator></eudc:creators><eudc:publishers><eudc:publisher>CDS</eudc:publisher></eudc:publishers><eudc:instruments/><eudc:publicationYear>2023</eudc:publicationYear><eudc:rightsList><eudc:rights>https://cds.unistra.fr/vizier-org/licences_vizier.html</eudc:rights></eudc:rightsList><eudc:fundingReferences/><eudc:contacts><eudc:contact>CDS support team &lt;cds-question@unistra.fr&gt;</eudc:contact></eudc:contacts><eudc:resourceTypes><eudc:resourceType>Dataset</eudc:resourceType><eudc:resourceType>AstroObjects</eudc:resourceType></eudc:resourceTypes><eudc:disciplines><eudc:discipline>astronomy</eudc:discipline></eudc:disciplines></eudc:resource></oai:metadata></oai:record></oai:GetRecord></oai:OAI-PMH>