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<ri:Resource created="2026-01-27T08:35:52Z" status="active" updated="2026-03-20T08:06:18Z" version="1.2" xmlns:cs="http://www.ivoa.net/xml/ConeSearch/v1.0" xmlns:ri="http://www.ivoa.net/xml/RegistryInterface/v1.0" xmlns:vr="http://www.ivoa.net/xml/VOResource/v1.0" xmlns:vs="http://www.ivoa.net/xml/VODataService/v1.1" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.ivoa.net/xml/ConeSearch/v1.0 http://vo.ari.uni-heidelberg.de/docs/schemata/ConeSearch.xsd http://www.ivoa.net/xml/VOResource/v1.0 http://vo.ari.uni-heidelberg.de/docs/schemata/VOResource.xsd http://www.ivoa.net/xml/VODataService/v1.1 http://vo.ari.uni-heidelberg.de/docs/schemata/VODataService.xsd" xsi:type="vs:CatalogService"><title>Microquasar V4641 Sgr image</title><shortName>J/A+A/706/A8</shortName><identifier>ivo://CDS.VizieR/J/A+A/706/A8</identifier><curation><publisher ivo-id="ivo://CDS">CDS</publisher><creator><name>Acharyya A.</name></creator><creator><name>Aharonian F.</name></creator><creator><name>Ashkar H.</name></creator><creator><name>Backes M.</name></creator><creator><name>Batzofin R.</name></creator><creator><name>Berge D.,Bernloehr K.</name></creator><creator><name>Boettcher M.</name></creator><creator><name>Boisson C.</name></creator><creator><name>Bolmont J.</name></creator><creator><name>Brun F.</name></creator><creator><name>Bruno B.,Burger-Scheidlin C.</name></creator><creator><name>Bylund T.</name></creator><creator><name>Casanova S.</name></creator><creator><name>Celic J.</name></creator><creator><name>Cerruti M.</name></creator><creator><name>Chen A.,Chernyakova M.</name></creator><creator><name>Chibueze J.O.</name></creator><creator><name>Chibueze O.</name></creator><creator><name>Cornejo B.</name></creator><creator><name>Cotter G.,de Assis Scarpin J.</name></creator><creator><name>de Bony de Lavergne M.</name></creator><creator><name>de Naurois M.,de Ona Wilhelmi E.</name></creator><creator><name>Delgado Giler A.G.</name></creator><creator><name>Devin J.</name></creator><creator><name>Djannati-Atai A.,Dmytriiev A.</name></creator><creator><name>Egberts K.</name></creator><creator><name>Egg K.</name></creator><creator><name>Ernenwein J.-P.</name></creator><creator><name>Escanuela Nieves C.,Fauverge P.</name></creator><creator><name>Feijen K.</name></creator><creator><name>Filipovic M.D.</name></creator><creator><name>Fontaine G.</name></creator><creator><name>Funk S.</name></creator><creator><name>Gabici S.,Gallant Y.A.</name></creator><creator><name>Glicenstein J.F.</name></creator><creator><name>Glombitza J.</name></creator><creator><name>Goswami P.</name></creator><creator><name>Grondin M.-H.,Heckmann L.</name></creator><creator><name>Hess B.</name></creator><creator><name>Hinton J.A.</name></creator><creator><name>Hofmann W.</name></creator><creator><name>Holch T.L.</name></creator><creator><name>Holler M.,Jamrozy M.</name></creator><creator><name>Jankowsky F.</name></creator><creator><name>Jardin-Blicq A.</name></creator><creator><name>Jaroschewski I.</name></creator><creator><name>Jimeno D.,Jung-Richardt I.</name></creator><creator><name>Katarzynski K.</name></creator><creator><name>Kerszberg D.</name></creator><creator><name>Khelifi B.</name></creator><creator><name>Komin N.,Kosack K.</name></creator><creator><name>Kostunin D.</name></creator><creator><name>Lang R.G.</name></creator><creator><name>Lazarevic S.</name></creator><creator><name>Lemiere A.,Lemoine-Goumard M.</name></creator><creator><name>Lenain J.-P.</name></creator><creator><name>Liniewicz P.</name></creator><creator><name>Luashvili A.</name></creator><creator><name>Mackey J.,Malyshev D.</name></creator><creator><name>Marandon V.</name></creator><creator><name>Mayer M.G.F.</name></creator><creator><name>Mehta A.</name></creator><creator><name>Mitchell A.M.W.,Moderski R.</name></creator><creator><name>Mohrmann L.</name></creator><creator><name>Montanari A.</name></creator><creator><name>Moulin E.</name></creator><creator><name>Niemiec J.,Olivera-Nieto L.</name></creator><creator><name>Moghadam M.O.</name></creator><creator><name>Panny S.</name></creator><creator><name>Parsons R.D.</name></creator><creator><name>Pensec U.,Pichard P.</name></creator><creator><name>Preis T.</name></creator><creator><name>Puehlhofer G.</name></creator><creator><name>Punch M.</name></creator><creator><name>Quirrenbach A.</name></creator><creator><name>Reimer A.,Reimer O.</name></creator><creator><name>Reis I.</name></creator><creator><name>Remy Q.</name></creator><creator><name>Ren H.X.</name></creator><creator><name>Reville B.</name></creator><creator><name>Rieger F.,Roellinghoff G.</name></creator><creator><name>Rowell G.</name></creator><creator><name>Rudak B.</name></creator><creator><name>Sabri K.</name></creator><creator><name>Safi-Harb S.</name></creator><creator><name>Sahakian V.,Santangelo A.</name></creator><creator><name>Sasaki M.</name></creator><creator><name>Schuessler F.</name></creator><creator><name>Shapopi J.N.S.</name></creator><creator><name>Si Said W.</name></creator><creator><name>Sol H.,Stawarz L.</name></creator><creator><name>Steinmassl S.</name></creator><creator><name>Tanaka T.</name></creator><creator><name>Taylor A.M.</name></creator><creator><name>Taylor G.L.</name></creator><creator><name>Terrier R.,Tian Y.</name></creator><creator><name>Timmermans A.</name></creator><creator><name>Tsirou M.</name></creator><creator><name>Tsuji N.</name></creator><creator><name>Unbehaun T.</name></creator><creator><name>van Eldik C.,Vecchi M.</name></creator><creator><name>Venter C.</name></creator><creator><name>Vink J.</name></creator><creator><name>Voitsekhovskyi V.</name></creator><creator><name>Wagner S.J.,Wierzcholska A.</name></creator><creator><name>Zacharias M.</name></creator><creator><name>Zdziarski A.A.</name></creator><creator><name>Zech A.</name></creator><creator><name>Zhong W.,H.E.S.S.Collaboration</name></creator><creator><name>Takekawa S.</name></creator><date role="Updated">2026-03-20T08:06:18Z</date><date role="Created">2026-01-27T08:35:52Z</date><contact><name>CDS support team</name><address>CDS, Observatoire de Strasbourg, 11 rue de l'Universite, F-67000 Strasbourg, France</address><email>cds-question@unistra.fr</email></contact></curation><content><subject>quasars</subject><subject>gamma-ray-astronomy</subject><description>Microquasars have emerged as promising candidates to explain the cosmic-ray flux at PeV energies. LHAASO observations reveal V4641 Sgr as the most extreme example so far, with a gamma-ray spectrum extending up to 800~TeV, requiring multi-PeV energy particles. The TeV emission is highly extended, challenging expectations given the reported low-inclination angle of the V4641 Sgr jets. We aim to spatially and spectrally resolve the gamma-ray emission from V4641 Sgr and investigate particle acceleration in the system. Using ~100h of H.E.S.S. data we perform a spectro-morphological study of the gamma-ray emission around V4641 Sgr. We employ HI and dedicated CO observations of the region to infer the presence of target material for cosmic-ray interactions. Multi-TeV emission around V4641 Sgr is detected with high significance. The emission region is elongated with major and minor axes: 0.34{deg}+/-0.04_stat_+/-0.01_syst_ and 0.06{deg}+/-0.01_stat_+/-0.01_syst_, respectively. A power-law spectrum with index ~1.8 is found and, together with results by other gamma-ray instruments, reveals for the first time a spectral energy distribution (SED) peaking at energies of ~100TeV. We find indications (3{sigma}) of a two-component morphology, with indistinguishable spectral properties. The position of V4641 Sgr is inconsistent with both the best-fit position of the single-component model and the dip between the two components. We find no significant evidence of energy-dependent morphology. No dense gas is found at any distance towards V4641 Sgr, placing an upper limit of n_gas_&lt;~0.2cm^-3^ within the gamma-ray emission region. The peak of the SED at ~100TeV identifies V4641 Sgr as a candidate cosmic-ray accelerator beyond the Knee. However, the absence of dense target gas places stringent energetic constraints on hadronic interpretations. The H.E.S.S. measurement requires an unusually hard (~1.5) spectral index for protons. A leptonic scenario faces fewer obstacles, provided particle transport is fast enough to avoid losses and reproduce the observed energy-independent morphology, though the absence of bright X-ray emission across the gamma-ray emission region requires a magnetic field strength &lt;~3muG. Our findings favour a leptonic origin of the gamma-ray emission. 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