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首页> 外文期刊>The Astrophysical journal >The Mass Distribution And Lifetime Of Prestellar Cores In Perseus, Serpens, And Ophiuchus
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The Mass Distribution And Lifetime Of Prestellar Cores In Perseus, Serpens, And Ophiuchus

机译:英仙座,Serpens和蛇夫座中星前核的质量分布和寿命

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摘要

We present an unbiased census of starless cores in Perseus, Serpens, and Ophiuchus, assembled by comparing large-scale Bolocam 1.1 mm continuum emission maps with Spitzer c2d surveys. We use the c2d catalogs to separate 108 starless from 92 protostellar cores in the 1.1 mm core samples from Enoch and Young and their coworkers. A comparison of these populations reveals the initial conditions of the starless cores. Starless cores in Perseus have similar masses but larger sizes and lower densities on average than protostellar cores, with sizes that suggest density profiles substantially flatter than ρ ∝ r~(-2). By contrast, starless cores in Serpens are compact and have lower masses than protostellar cores; future star formation will likely result in lower mass objects than the currently forming protostars. Comparison to dynamical masses estimated from the NH_3 survey of Perseus cores by Rosolowsky and coworkers suggests that most of the starless cores are likely to be gravitationally bound, and thus prestellar. The combined prestellar core mass distribution includes 108 cores and has a slope of α = -2.3 ± 0.4 for M > 0.8 M_☉. This slope is consistent with recent measurements of the stellar initial mass function, providing further evidence that stellar masses are directly linked to the core formation process. We place a lower limit on the core-to-star efficiency of 25%. There are approximately equal numbers of prestellar and protostellar cores in each cloud; thus the dense prestellar core lifetime must be similar to the lifetime of embedded protostars, or 4.5 × 10~5 yr, with a total uncertainty of a factor of 2. Such a short lifetime suggests a dynamic, rather than quasi-static, core evolution scenario, at least at the relatively high mean densities (n > 2 × 10~4 cm~(-3)) to which we are sensitive.
机译:我们通过比较大型Bolocam 1.1毫米连续体发射图和Spitzer c2d测量结果,对珀尔修斯,塞尔彭斯和蛇夫座的无星核进行了无偏差普查。我们使用c2d目录在来自Enoch和Young及其同事的1.1毫米岩心样本中将92个原恒星核中的108个无恒星核分开。这些种群的比较揭示了无星核的初始条件。英仙座中的无恒星核具有相似的质量,但平均大小比原恒星核大,密度也较低,其大小表明密度分布比ρr〜(-2)基本平坦。相比之下,瑟彭斯的无恒星核心是紧凑的,并且质量比恒星核心低。未来的恒星形成可能会导致质量比当前形成的原恒星低的物体。 Rosolowsky及其同事根据NH_3对英仙座核进行的NH_3调查所估计的动力质量的比较表明,大多数无恒星核很可能受到引力束缚,因此是星前的。合并的星前核心质量分布包括108个核心,并且当M> 0.8M_☉时,斜率为α= -2.3±0.4。该斜率与最近对恒星初始质量函数的测量结果一致,进一步证明了恒星质量与岩心形成过程直接相关。我们将核心到星级效率的下限设置为25%。每个云中大约有相等数量的星前和原恒星核心。因此,密集的恒星核心寿命必须与嵌入式原恒星的寿命相近,即4.5×10〜5年,总不确定度约为2。如此短的寿命暗示着动态的而不是准静态的核心演化情况下,至少在我们敏感的相对较高的平均密度(n> 2×10〜4 cm〜(-3))下。

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