2009
DOI: 10.1051/0004-6361/200912659
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Hot stars observed by XMM-Newton

Abstract: Aims. Following the advent of increasingly sensitive X-ray observatories, deep observations of early-type stars became possible. However, the results for only a few objects or clusters have until now been reported and there has been no large survey comparable to that based upon the ROSAT All-Sky Survey (RASS). Methods. A limited survey of X-ray sources, consisting of all public XMM-Newton observations (2XMMi) and slew survey data (XMMSL1), is now available. The X-ray counterparts to hot, massive stars have bee… Show more

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Cited by 144 publications
(199 citation statements)
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“…Both these findings strongly suggest that BD +37 ∘ 442 is a single star without any companion and that the observed X-ray emission originates from the sdO star itself. This hypothesis is supported by other data: the estimated X-ray luminosity implies an X-ray-to-bolometric ratio L X / L BOL ∼ 2 × 10 −7 , a value consistent with the average relation observed in normal O-type stars; we already know from UV and optical spectroscopy that this star is characterized by a significant stellar wind (Jeffery & Hamann 2010); finally, the estimated plasma temperature is comparable to the lowest values seen in the sample of O-type stars observed with XMM-Newton (Nazé 2009). Therefore, we conclude that the observed X-ray emission is most probably related to the shock-heated plasma produced by instabilities in the radiation-driven stellar wind of the sdO star.…”
Section: New Results On Hd 49798: Pulsar Spin-up and Intrinsic X-ray supporting
confidence: 80%
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“…Both these findings strongly suggest that BD +37 ∘ 442 is a single star without any companion and that the observed X-ray emission originates from the sdO star itself. This hypothesis is supported by other data: the estimated X-ray luminosity implies an X-ray-to-bolometric ratio L X / L BOL ∼ 2 × 10 −7 , a value consistent with the average relation observed in normal O-type stars; we already know from UV and optical spectroscopy that this star is characterized by a significant stellar wind (Jeffery & Hamann 2010); finally, the estimated plasma temperature is comparable to the lowest values seen in the sample of O-type stars observed with XMM-Newton (Nazé 2009). Therefore, we conclude that the observed X-ray emission is most probably related to the shock-heated plasma produced by instabilities in the radiation-driven stellar wind of the sdO star.…”
Section: New Results On Hd 49798: Pulsar Spin-up and Intrinsic X-ray supporting
confidence: 80%
“…For all stars the detected X-ray fluxes are very low (f X ∼ 10 −14 erg cm −2 s −1 ); they imply L X = 10 30−31 and 10 28−29 erg s −1 for the 'luminous' and 'compact' stars, respectively. Two results suggest that also for these subdwarf stars the observed X-ray emission originates in the stellar wind: in all cases the X-ray/bolometric flux ratio is ∼ 10 −7 , in agreement with the relation found for the massive early-type stars; both the spectra of BD +37 ∘ 442 (Mereghetti et al 2017) and BD +37 ∘ 1977(La Palombara et al 2015 were well described with the sum of two plasma emission models with different temperatures, as in the case of the massive stars (Nazé 2009). …”
Section: Introductionsupporting
confidence: 86%
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“…The temperature found in the spectral fits of BD +37 • 442 is in the lower range of the values seen in the sample of O-type stars observed with the XMM-Newton EPIC instrument, when a singletemperature plasma is sufficient to describe their low resolution Xray spectra (Nazé 2009). This might be related to the weaker wind of BD +37 • 442 compared to that of normal O-type stars.…”
Section: Discussionmentioning
confidence: 71%
“…X-rays are produced in the winds of single stars by shockheated plasma resulting from various instabilities (see, e.g., Oskinova 2016, and references therein). An empirical correlation has been found between the X-ray and bolometric luminosities of early type stars: L X ∼ 10 −7 L BOL (Pallavicini et al 1981;Nazé 2009). The X-ray luminosity we derived for BD +37 • 442 corresponds to a value of L X /L BOL ∼ 2 × 10 −7 , fully consistent with the observed dispersion around the above average relation.…”
Section: Discussionmentioning
confidence: 93%