2016
DOI: 10.3847/2041-8205/826/2/l26
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An Iron K Component to the Ultrafast Outflow in NGC 1313 X-1

Abstract: We present the detection of an absorpton feature at E = 8.77 +0.05 −0.06 keV in the combined X-ray spectrum of the ultraluminous X-ray source NGC 1313 X-1 observed with XMM-Newton and NuSTAR, significant at the 3σ level. If associated with blueshifted ionized iron, the implied outflow velocity is ∼0.2c for Fe XXVI, or ∼0.25c for Fe XXV. These velocities are similar to the ultrafast outflow seen in absorption recently discovered in this source at lower energies by XMM-Newton, and we therefore conclude that this… Show more

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Cited by 116 publications
(170 citation statements)
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References 50 publications
(67 reference statements)
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“…Last, we also revisit the limits on the presence of any atomic iron absorption or emission features in light of the ultra-fast outflow (∼0.2-0.25c) recently detected in NGC 1313 X-1 Walton et al 2016b). The high-energy constraints provided by the NuSTAR data, missing in our previous line searches for Holmberg IX X-1 (Walton et al 2012(Walton et al , 2013b), mean we can now significantly improve our sensitivity to any features associated with high-velocity outflows for this source.…”
Section: Fe K Line Searchmentioning
confidence: 90%
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“…Last, we also revisit the limits on the presence of any atomic iron absorption or emission features in light of the ultra-fast outflow (∼0.2-0.25c) recently detected in NGC 1313 X-1 Walton et al 2016b). The high-energy constraints provided by the NuSTAR data, missing in our previous line searches for Holmberg IX X-1 (Walton et al 2012(Walton et al , 2013b), mean we can now significantly improve our sensitivity to any features associated with high-velocity outflows for this source.…”
Section: Fe K Line Searchmentioning
confidence: 90%
“…Considering the XMM-Newton, Suzaku, and NuSTAR databases, the majority of the archival exposure available for Holmberg IX X-1 covers states similar to epoch 1, so we focus on these data in order to maximize the S/N while considering only observations with similar spectra. Following Walton et al (2016b), we also only consider XMMNewton observations in which Holmberg IX X-1 was placed on-axis in order to avoid increased background emission from copper lines at ∼8 keV seen in the EPIC-pn detector away from the optical axis (Carter & Read 2007), which fall in the energy range of interest. Therefore, in addition to the data from epochs 1, 3, and 6, we also include archival data from anotherlong Suzaku exposure (OBSID 707019010)and two short XMMNewton exposures (ODSIDs 0112521001 and 0112521101).…”
Section: Fe K Line Searchmentioning
confidence: 99%
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“…From Figure 4 it is clear that the strongest spectral change is observed in p. At super-Eddington accretion rates, it is expected that the accretion disk is flared up due to radiation pressure, i.e., itbecomes geometrically thick and increases in size with radius. In addition, a strong wind is launched, which is also largely optically thick (Poutanen et al 2007;Dotan & Shaviv 2011) and for which observational evidence has recently been found in NGC 1313X-1 and NGC 5408X-1 (Pinto et al 2016;Walton et al 2016b). The observed temperature profile, therefore, depends on which parts and with what angle we observe the accretion disk.…”
Section: Connection Between the Super-orbital Period And Spectral Chamentioning
confidence: 99%