论文标题
Illustristng模拟中的禁止星系
Barred Galaxies in the IllustrisTNG Simulation
论文作者
论文摘要
当地宇宙宿主杆中,几乎三分之二的磁盘星系是世俗进化过程的重要驱动因素。尽管宇宙学模拟是研究星系形成和演变的强大工具,但他们经常努力产生合理的酒吧种群。我们测量了高级宇宙模拟Illustristng的TNG100运行中3866个磁盘星系中条形线的分数,大小和强度。与观察结果一致,约有55%的磁盘星系具有恒星质量$ M_* \约10^{10.6} \,M_ \ odot $被禁止使用,并且条尺寸和总恒星质量之间的关系与在近乎汇率的监视中相似。但是,在带有$ M_* <10^{10.6} \,M_ \ odot $的星系中抑制条形的形成,这可能是由于TNG100难度在解决半径<1.4 kpc的短条中造成的。相比之下,$ M_*> 10^{10.6} \,M_ \ odot $具有$ M_*> 10^{10.6} \ odot $的大型磁盘星系中多达75%的磁盘星系,比观察到的酒吧高约10%-20%。相对于在近红外调查中观察到的质量杆尺寸关系,TNG100过度产生了相对较短的条(半径〜1.4-3 kpc)。追踪Z = 0的祖细胞大量星系,我们发现条形分数从z = 1和0之间的25%增加到63%。相反,如果我们在z = 0-1中选择所有磁盘星系,并且恒定地降低了$ m_* \ geqslant 10^{10.6} {10.6}} \,m_ \ odot $,我们会发现bar fratairs bar fratairs是一个常数60%。
Almost two-thirds of disk galaxies in the local universe host bars, which serve as important drivers of secular evolutionary processes. While cosmological simulations are powerful tools to study the formation and evolution of galaxies, they have often struggled to generate reasonable bar populations. We measure the fraction, size, and strength of bars in 3866 disk galaxies from the TNG100 run of the advanced cosmological simulation IllustrisTNG. Consistent with observations, about 55% of disk galaxies with stellar mass $M_* \approx 10^{10.6}\, M_\odot$ are barred, and the relation between bar size and total stellar mass is similar to that found in near-infrared surveys. However, the formation of bars is suppressed in galaxies with $M_* < 10^{10.6}\, M_\odot$, which may result from the difficulty TNG100 has in resolving short bars with radius <1.4 kpc. In contrast, up to 75% of massive disk galaxies with $M_* > 10^{10.6}\, M_\odot$ have bars, ~10%-20% higher than observed. TNG100 overproduces relatively short bars (radius ~1.4-3 kpc) with respect to the mass-bar size relation observed in near-infrared surveys. Tracing the progenitors of z=0 massive galaxies we find that the bar fraction increases from 25% to 63% between z=1 and 0. Instead if we select all disk galaxies during z=0-1 with a constant mass cut of $M_* \geqslant 10^{10.6}\, M_\odot$ we find that the bar fraction is a nearly constant 60%.