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arXiv 1408.1102astro-ph.GAastro-ph.CO
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暖暗物质宇宙学中早期星系形成

Early galaxy formation in warm dark matter cosmologies

Pratika Dayal, Andrei Mesinger, Fabio Pacucci

摘要:

我们提出了一个高红移($z \geq 7$)星系形成的框架,跟踪他们的暗物质(DM)和重子组装在四个宇宙学:冷暗物质(CDM)和暖暗物质(WDM)与粒子质量的$m_x =$ 1.5,3和5 ${\rm keV}$。我们使用相同的天体物理参数调节恒星的形成和反馈,选择匹配不断变化的紫外线光度函数(UV LF)的当前观测。我们发现CDM和$m_x \geq 3 {\rm keV}$ WDM中的可观测星系(使用当前和即将到来的仪器)的组装导致相似的晕质光比(M/L),恒星质量密度(SMD)和UV LF。然而,在$1.5 {\rm keV}$ WDM模型中,对小尺度结构的抑制导致了一个明显的延迟和随后更快的恒星组装。因此,在$m_x \leq 2 {\rm keV}$ WDM宇宙学的星系大会的特点是:(一)缺乏小质量的晕托管微弱的星系;(二)年轻,更紫外线明亮的恒星人口,对于一个给定的恒星质量。较高的M/L比(效果ii)部分补偿了小质量晕的缺乏(效果i),使所得的紫外线LF更接近CDM比从简单的估计晕丰度。我们发现SMD的红移演化是对DM性质的一个强有力的探测。对于詹姆斯·韦伯太空望远镜(JWST),积分到$M_{UV} =-16.5$的极限,SMD在$m_x = 1.5 {\rm keV}$ WDM中演化为$\log$(SMD)$\propto -0.63 (1+z)$,而在CDM中演化为$\log$(SMD)$\propto -0.44 (1+z)$。因此,高红移恒星组装提供了一个强大的测试平台WDM模型,即将到来的JWST访问。

英文摘要:

We present a framework for high-redshift ($z \geq 7$) galaxy formation that traces their dark matter (DM) and baryonic assembly in four cosmologies: Cold Dark Matter (CDM) and Warm Dark Matter (WDM) with particle masses of $m_x =$ 1.5, 3 and 5 ${\rm keV}$. We use the same astrophysical parameters regulating star formation and feedback, chosen to match current observations of the evolving ultra violet luminosity function (UV LF). We find that the assembly of observable (with current and upcoming instruments) galaxies in CDM and $m_x \geq 3 {\rm keV}$ WDM results in similar halo mass to light ratios (M/L), stellar mass densities (SMDs) and UV LFs. However the suppression of small-scale structure leads to a notably delayed and subsequently more rapid stellar assembly in the $1.5 {\rm keV}$ WDM model. Thus galaxy assembly in $m_x \leq 2 {\rm keV}$ WDM cosmologies is characterized by: (i) a dearth of small-mass halos hosting faint galaxies; and (ii) a younger, more UV bright stellar population, for a given stellar mass. The higher M/L ratio (effect ii) partially compensates for the dearth of small-mass halos (effect i), making the resulting UV LFs closer to CDM than expected from simple estimates of halo abundances. We find that the redshift evolution of the SMD is a powerful probe of the nature of DM. Integrating down to a limit of $M_{UV} =-16.5$ for the James Webb Space Telescope (JWST), the SMD evolves as $\log$(SMD)$\propto -0.63 (1+z)$ in $m_x = 1.5 {\rm keV}$ WDM, as compared to $\log$(SMD)$\propto -0.44 (1+z)$ in CDM. Thus high-redshift stellar assembly provides a powerful testbed for WDM models, accessible with the upcoming JWST.

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