A possible solution to the [a/Fe]-s problem in early-type galaxies within a hierarchical galaxy formation model The [a/Fe]-s problem in early-type galaxies
A possible solution to the [a/Fe]-s problem in early-type galaxies within a hierarchical galaxy formation model The [a/Fe]-s problem in early-type galaxies
复制标题
分层星系形成模型中早期型星系中 [a/Fe]-s 问题的一种可能解决方案 早期型星系中的 [a/Fe]-s 问题
DOI:
10.1111/j.1745-3933.2011.01017.x
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发表时间:
2011
期刊:
影响因子:
--
通讯作者:
Calura F
中科院分区:
文献类型:
--
作者:
Calura F
The most massive elliptical galaxies apparently formed the fastest, because the ratio of α elements (such as oxygen) to iron is the smallest. In fact, iron is mainly produced from type Ia supernovae on a time-scale of ∼0.1–1 Byr, while the α elements come from massive stars on time-scales of a few tens of million years. Reproducing such a α/Fe correlation has long been a severe problem for cosmological theories of galaxy formation, which envisage massive galaxies to assemble gradually from smaller progenitors, and to be characterized by a star formation history too much extended towards late cosmic times. While it has recently become clear that feedback from Active Galactic Nuclei (AGNs) activity plays a role in the late quenching of star formation, and that early star formation history in the galaxy progenitors affect the α/Fe ratio, major mergers alone cannot enhance the star formation in the high-redshift progenitors to the levels required to match the steepness of the observed α/Fe correlation. Here we report that the inclusion of the effects of fly-by ‘harassments’, that trigger lower level starbursts, combined with the AGN quenching of the starburst activity, considerably enhances the capability to account for the observed α/Fe ratio in ellipticals within cosmological galaxy formation models. The critical difference between the earlier work and the present result is the effect of starbursts driven by fly-by encounters that would have been very common amongst the high-redshift progenitors of massive galaxies and which would have boosted star formation in the first 2 Byr after the big bang, combined with quenching of the burst activity within the first 3–4 Gyr.