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arXiv 1901.01192astro-ph.GA
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从爆发指示器的分布测量恒星形成的随机性

Star Formation Stochasticity Measured from the Distribution of Burst Indicators

Adam Broussard, Eric Gawiser, Kartheik Iyer, Peter Kurczynski, Rachel S. Somerville, Romeel Davé, Steve Finkelstein, Intae Jung, Camilla Pacifici

摘要:

理解星系形成和演化的关键问题之一是恒星暴增如何影响星系中恒星星族随时间的聚集。我们定义了一个爆发指标($η$),它比较了一个星系的恒星形成率短($\sim10$ Myr)和长($\sim100$ Myr)的时间尺度。为了估计$η$,我们应用H $α$和近紫外辐射的详细时间-光度关系,从半解析模型和Mufasa流体动力学宇宙学模拟模拟的恒星形成历史(SFHS)。$η$的平均值并不是恒星形成随机性(突发性)的一个很好的指标;事实上,我们表明,这个平均值应该接近于零,除非人口的平均SFH正在迅速上升或下降。相反,$η$分布的宽度表征了星系群最近恒星形成的爆发性。我们发现这个宽度是强大的恒星初始质量函数和金属丰度的变化。我们应用现实的噪声和选择效应的模型,以产生模拟HST和JWST星系目录和比较这些目录与3D-HST观测的956个星系在$0.65<z<1.5$检测H $α$。在假设$η$(即,$Q_\mathrm{sg}=0.44$)。然而,设置$Q_\mathrm{sg}=0.8^{+0.1}_{-0.2}$可以消除3D-HST样本中$η$的平均值对尘埃衰减和恒星质量的意外依赖,同时还可以解决恒星形成率分布中的分歧。然而,即使改变尘埃定律也不能解决模拟星系和观测星系之间的所有差异。

英文摘要:

One of the key questions in understanding the formation and evolution of galaxies is how starbursts affect the assembly of stellar populations in galaxies over time. We define a burst indicator ($η$), which compares a galaxy's star formation rates on short ($\sim10$ Myr) and long ($\sim100$ Myr) timescales. To estimate $η$, we apply the detailed time-luminosity relationship for H$α$ and near-ultraviolet emission to simulated star formation histories (SFHs) from semi-analytic models and the Mufasa hydrodynamical cosmological simulations. The average of $η$ is not a good indicator of star formation stochasticity (burstiness); indeed, we show that this average should be close to zero unless the population has an average SFH which is rising or falling rapidly. Instead, the width of the $η$ distribution characterizes the burstiness of a galaxy population's recent star formation. We find this width to be robust to variations in stellar initial mass function and metallicity. We apply realistic noise and selection effects to the models to generate mock HST and JWST galaxy catalogs and compare these catalogs with 3D-HST observations of 956 galaxies at $0.65<z<1.5$ detected in H$α$. Measurements of $η$ are unaffected by dust measurement errors under the assumption that $E(B-V)_\mathrm{stars}=0.44\,E(B-V)_\mathrm{gas}$ (i.e., $Q_\mathrm{sg}=0.44$). However, setting $Q_\mathrm{sg}=0.8^{+0.1}_{-0.2}$ removes an unexpected dependence of the average value of $η$ upon dust attenuation and stellar mass in the 3D-HST sample while also resolving disagreements in the distribution of star formation rates. However, even varying the dust law cannot resolve all discrepancies between the simulated and the observed galaxies.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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