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Carbon and oxygen isotope ratios in starburst galaxies: New data from NGC 253 and Mrk 231 and their implications

机译:星爆星系中的碳氧同位素比:来自NGC 253和Mrk 231的新数据及其含义

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Carbon and oxygen isotope ratios are excellent measures of nuclear processing, but few such data have been taken toward extragalactic targets so far. Therefore, using the IRAM 30-m telescope, CN and CO isotopologues have been measured toward the nearby starburst galaxy NGC 253 and the prototypical ultraluminous infrared galaxy Mrk 231. Toward the center of NGC 253, the CN and 13CN N = 1 → 0 lines indicate no significant deviations from expected local thermodynamical equilibrium after accounting for moderate saturation effects (10 and 25%) in the two detected spectral components of the main species. Including calibration uncertainties, which dominate the error budget, the 12C/13C ratio becomes 40?±?10. This is larger than the ratio in the central molecular zone of the Galaxy, suggesting a higher infall rate of poorly processed gas toward the central region. Assuming that the ratio also holds for the CO emitting gas, this yields 16O/18O = 145?±?36 and 16O/17O = 1290?±?365 and a 32S/34S ratio close to the one measured for the local interstellar medium (20–25). No indication of vibrationally excited CN is found in the lower frequency fine structure components of the N = 1 → 0 and 2 → 1 transitions at rms noise levels of 3 and 4?mK (15 and 20?mJy) in 8.5?km?s-1 wide channels. Peak line intensity ratios between NGC 253 and Mrk 231 are ~100 for 12C16O and 12C18O J = 1 → 0, while the ratio for 13C16O J = 1 → 0 is ~250. This and similar 13CO and C18O line intensities in the J = 1 → 0 and 2 → 1 transitions of Mrk 231 suggest 12C/13C ~ 100 and 16O/18O ~ 100, in agreement with values obtained for the less evolved ultraluminous merger Arp 220. Also, when accounting for other (scarcely available) extragalactic data, 12C/13C ratios appear to vary over a full order of magnitude, from >100 in ultraluminous high redshift galaxies to ~100 in more local such galaxies to ~40 in weaker starbursts that are not undergoing a large scale merger to 25 in the central molecular zone of the Milky Way. With 12C being predominantly synthesized in massive stars, while 13C is mostly ejected by longer lived lower mass stars at later times, this is qualitatively consistent with our results of decreasing carbon isotope ratios with time and rising metallicity. It is emphasized, however, that both infall of poorly processed material, initiating a nuclear starburst, and the ejecta from newly formed massive stars (in particular in the case of a top-heavy stellar initial mass function) can raise the carbon isotope ratio for a limited amount of time.
机译:碳和氧的同位素比是核加工的极好方法,但迄今为止,很少有这样的数据用于河外目标。因此,使用IRAM 30-m望远镜,已向附近的星爆星系NGC 253和典型的超发光红外星系Mrk 231测量了CN和CO同位素。朝NGC 253的中心,CN和13CN N = 1→0线表明在考虑了主要物种的两个检测到的光谱成分中的中等饱和效应(分别为10%和25%)之后,与预期的局部热力学平衡没有明显差异。包括校准误差在内的校准不确定度,误差在12C / 13C之内变为40?±?10。这大于银河中央分子区域的比率,表明处理不良的气体向中央区域的流入率更高。假设该比率也适用于CO排放气体,则得出16O / 18O = 145?±?36和16O / 17O = 1290?±?365,并且32S / 34S的比率接近于本地星际介质所测得的比率( 20–25)。在8.5?km?s的rms噪声水平为3和4?mK(15和20?mJy)时,N = 1→0和2→1过渡的低频精细结构分量中没有发现振动激发的CN的迹象。 -1个广泛的渠道。对于12C16O和12C18O J = 1→0,NGC 253和Mrk 231之间的峰线强度比为〜100,而对于13C16O J = 1→0的峰线强度比为〜250。在Mrk 231的J = 1→0和2→1跃迁中,此和类似的13CO和C18O谱线强度表明12C / 13C〜100和16O / 18O〜100,与进化较少的超发光合并Arp 220的值一致。同样,当考虑其他(很少可用)河外数据时,12C / 13C比似乎在整个数量级上变化,从超发光高红移星系的> 100到更局部的此类星系的〜100,到较弱的星爆的〜40在银河系的中央分子区域没有大规模合并到25。由于12C主要在大质量恒星中合成,而13C主要是在较晚的时间由寿命更长的低质量恒星排出,这在质量上与我们随时间降低碳同位素比和提高金属度的结果一致。但是要强调的是,加工不良的材料的注入(引发核爆炸)和新形成的大质量恒星的喷射(特别是在顶部重的恒星初始质量函数的情况下)都可以提高碳同位素比。有限的时间。

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