2004
DOI: 10.1086/422181
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Confronting the Superbubble Model with X‐Ray Observations of 30 Doradus C

Abstract: We present an analysis of XMM-Newton observations of the superbubble 30 Dor C and compare the results with the predictions from the standard wind-blown bubble model. We find that the observed X-ray spectra cannot be fitted satisfactorily with the model alone and that there is evidence for nonthermal X-ray emission, which is particularly important at k4 keV. The combination of the bubble model and a power law gives a reasonable fit to the observed spectra. The thermal pressure and central temperature of the bub… Show more

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Cited by 34 publications
(46 citation statements)
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“…Simple formulas for thermal evaporation in the absence of magnetic fields (Cowie et al 1981) and cloud destruction by hydrodynamic ablation (Klein et al 1994;Poludnenko et al 2002) show that small clouds of size 1 pc and density 100 cm À2 can survive for a time of order 10 6 yr in a wind fluid of density 10 À3 cm À2 and temperature 3 ; 10 7 K. This is not much smaller than the wind lifetime (5 ; 10 6 5 ; 10 7 yr) of a 5 kpc shell with a constant velocity of 100-1000 km s À1 . Various effects can increase cloud lifetimes, including (1) the presence of azimuthal magnetic fields, which make cloud evaporation less likely, as they decrease conduction relative to the classical Spitzer value (as observed in 30 Dor; Smith & Wang 2004); (2) conversely, increased heat conduction, which may inhibit hydrodynamic instabilities ( Marcolini et al 2005); (3) clouds stop evaporating when they are crushed to high optical depth (Ferrara & Shchekinov 1993); and (4) Kelvin-Helmholtz instabilities are suppressed by ablation of small bumps in the cloud (Schiano et al 1995). Cloud lifetimes can be decreased, however, by interactions among nearby clouds (Poludnenko et al 2004).…”
Section: Wind Geometry Cloud Lifetimes and Time-averagingmentioning
confidence: 99%
“…Simple formulas for thermal evaporation in the absence of magnetic fields (Cowie et al 1981) and cloud destruction by hydrodynamic ablation (Klein et al 1994;Poludnenko et al 2002) show that small clouds of size 1 pc and density 100 cm À2 can survive for a time of order 10 6 yr in a wind fluid of density 10 À3 cm À2 and temperature 3 ; 10 7 K. This is not much smaller than the wind lifetime (5 ; 10 6 5 ; 10 7 yr) of a 5 kpc shell with a constant velocity of 100-1000 km s À1 . Various effects can increase cloud lifetimes, including (1) the presence of azimuthal magnetic fields, which make cloud evaporation less likely, as they decrease conduction relative to the classical Spitzer value (as observed in 30 Dor; Smith & Wang 2004); (2) conversely, increased heat conduction, which may inhibit hydrodynamic instabilities ( Marcolini et al 2005); (3) clouds stop evaporating when they are crushed to high optical depth (Ferrara & Shchekinov 1993); and (4) Kelvin-Helmholtz instabilities are suppressed by ablation of small bumps in the cloud (Schiano et al 1995). Cloud lifetimes can be decreased, however, by interactions among nearby clouds (Poludnenko et al 2004).…”
Section: Wind Geometry Cloud Lifetimes and Time-averagingmentioning
confidence: 99%
“…The hot gas is enriched in α-elements (O, Ne, Mg, Si, S, Ar, Ca) by a factor of about 3 while the group of Fe-like elements is consistent with the LMC abundances. The additional ≃ 5 M ⊙ of oxygen in the hot gas require 2-3 high mass (≥ 20 M ⊙ ) recent core-collapse supernovae (Smith & Wang 2004). Nonthermal emission has been detected as well in this superbubble (Bamba et al 2004).…”
Section: Superbubblesmentioning
confidence: 70%
“…Why the amount of energy currently present in superbubbles is significantly less than the energy input expected from the enclosed massive stars over their lifetime (Cooper et al 2004)? What is the origin of the nonthermal emission observed in some superbubbles (Smith & Wang 2004)? Are superbubbles a relevant source for the acceleration of galactic cosmic rays (Parizot et al 2004)?…”
Section: Superbubblesmentioning
confidence: 99%
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“…A remarkable feature of the X-ray emission from N 51D is that its X-ray spectrum requires a nonthermal component to explain the emission in 1−3 keV. Nonthermal X-ray emission has also been detected in the LMC superbubbles 30 Dor C (Bamba et al 2004;Smith & Wang 2004) and N 11 (Maddox et al 2008). N 51D does not have detectable molecular clouds around its superbubble shell rim; however, there is still on-going star formation.…”
Section: Energy Feedback and Star Formation In Superbubblesmentioning
confidence: 99%