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arXiv 2404.08033astro-ph.COastro-ph.GAastro-ph.SR
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利用红移$z\approx1$的透镜化恒星在最小尺度上对暗物质成像

Imaging dark matter at the smallest scales with $z\approx1$ lensed stars

J. M. Diego, Sung Kei Li, Alfred Amruth, Ashish K. Meena, Tom J. Broadhurst, Patrick L. Kelly, Alexei V. Filippenko, Liliya L. R. Williams, Adi Zitrin, William … 展开作者

J. M. Diego, Sung Kei Li, Alfred Amruth, Ashish K. Meena, Tom J. Broadhurst, Patrick L. Kelly, Alexei V. Filippenko, Liliya L. R. Williams, Adi Zitrin, William E. Harris, Marta Reina-Campos, Carlo Giocoli, Liang Dai, Mitchell F. Struble, Tommaso Treu, Yoshinobu Fudamoto, Daniel Gilman, Anton M. Koekemoer, Jeremy Lim, J. M. Palencia, Fengwu Sun, Rogier A. Windhorst

AI总结:

本研究针对星系团远区微引力透镜事件偏多的问题,通过3M透镜效应分析,发现光度函数形状与子结构共同决定事件分布,提出可利用事件数密度对小尺度暗物质成像,并在Dragon弧中发现可能的暗物质子结构证据。

摘要:

对红移$0.7<z<1$的焦散面穿越星系的观测显示存在大量暂现事件,其中大多数被认为是高放大率恒星的微引力透镜事件。早期研究预测这类事件在星系团的临界曲线(CCs)附近应较为常见,但部分事件被发现距离这些临界曲线相对较远。我们考虑了毫角秒尺度(透镜平面内为几秒差距)的子结构增强微引力透镜信号的可能性,研究了来自宏观透镜、毫透镜和微透镜的联合放大效应(3M透镜效应)。在考虑了符合实际的毫透镜与微透镜星族后,我们得出结论:毫透镜周围增强的微引力透镜事件率不足以解释远区观测到的高事件占比。相反,我们发现透镜化恒星的光度函数(LF)形状与透镜平面内的子结构数量共同决定了在临界曲线附近和远处发现的微引力透镜事件数量。通过测量$\beta$(光度函数的指数)以及每个位置的微引力透镜事件数密度,我们可以构建小尺度下潜在质量分布的伪图像。我们确定了两种机制:(i)正成像机制,即$\beta>2$时,子结构周围的事件数密度更高;(ii)负成像机制,即$\beta<2$时。我们研究了哈勃空间望远镜(HST)在Dragon弧(红移z=0.725)中发现的7个微引力透镜事件的具体案例,发现具有陡峭光度函数($\beta=2.55$)的超巨星星族能够拟合这些事件的分布。我们识别出一个微引力透镜事件高密度的小区域,并将其解释为可能存在不可见子结构的证据,我们推算出该子结构(在其爱因斯坦半径内)的质量约为$1.3 \times 10^8\\,\Msun$。

英文摘要:

Observations of caustic-crossing galaxies at redshift $0.7<z<1$ show a wealth of transient events. Most of them are believed to be microlensing events of highly magnified stars. Earlier work predicted such events should be common near the critical curves (CCs) of galaxy clusters, but some are found relatively far away from these CCs. We consider the possibility that substructure on milliarcsecond scales (few parsecs in the lens plane) is boosting the microlensing signal. We study the combined magnification from the macrolens, millilenses, and microlenses (3M-lensing). After considering realistic populations of millilenses and microlenses, we conclude that the enhanced microlensing rate around millilenses is not sufficient to explain the high fraction of observed events in the far region. Instead we find a that the shape of the luminosity function (LF) of the lensed stars combined with the amount of substructure in the lens plane determines the number of mcirolensing events found near and far from the CC. By measuring $β$ (the exponent of the LF), and the number density of microlensing events at each location, one can create a pseudoimage of the underlying distribution of mass on small scales. We identify two regimes: (i) positive imaging regime where $β>2$ and the number density of events is greater around substructureand the number density of events is greater around substructures, and (ii) negative imaging regime where $β<2$. We study the particular case of seven microlensing events found by HST in the Dragon arc (at z=0.725). We find that a population of supergiant stars with a steep LF with $β=2.55$ fits the distribution of these events. We identify a small region of high density of microlensing events, and interpret it as evidence of a possible invisible substructure, for which we derive a mass of $\sim 1.3 \times 10^8\,\Msun$ (within its Einstein radius).

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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