首页> 外文期刊>The Astrophysical journal >OBSERVATIONS OF DENSE MOLECULAR GAS IN A QUASAR HOST GALAXY AT z = 6.42: FURTHER EVIDENCE FOR A NONLINEAR DENSE GAS-STAR FORMATION RELATION AT EARLY COSMIC TIMES
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OBSERVATIONS OF DENSE MOLECULAR GAS IN A QUASAR HOST GALAXY AT z = 6.42: FURTHER EVIDENCE FOR A NONLINEAR DENSE GAS-STAR FORMATION RELATION AT EARLY COSMIC TIMES

机译:在z = 6.42时的拟态宿主星系中的稠密分子气的观测:早宇宙时间非线性稠密气-星形成关系的进一步证据

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We report a sensitive search for the HCN(J = 2 → 1) emission line toward SDSS J114816.64+525150.3 (hereafter J1148+5251) at z = 6.42 with the Very Large Array (VLA). HCN emission is a star formation indicator, tracing dense molecular hydrogen gas [n(H_2) ≥ 10~4 cm~(-3)] within star-forming molecular clouds. No emission was detected in the deep interferometer maps of J1148+5251. We derive a limit for the HCN line luminosity of L′_(HCN) < 3.3 × 10~9 K km s~(-1) pc~2, corresponding to a HCN/CO luminosity ratio of L′_(HCN)/L′_(CO) < 0.13. This limit is consistent with a fraction of dense molecular gas in J1148+5251 within the range of nearby ultraluminous infrared galaxies (ULIRGs; median value: L′_(HCN)/L′_(CO) = 0.17_(-0.08)~(+0.05) and HCN-detected z > 2 galaxies (0.17_(-0.08)~(+0.09)). The relationship between L′_(HCN) and L_(FIR) is considered to be a measure of the efficiency at which stars form out of dense gas. In the nearby universe, these quantities show a linear correlation, and thus, a practically constant average ratio. In J1148 + 5251, we find L_(FIR)/L′_(HCN) > 6600. This is significantly higher than the average ratios for normal nearby spiral galaxies (L_(FIR)/L′_(HCN) = 580_(-270)~(+510) and ULIRGs (740_(-50)~(+505)), but consistent with a rising trend as indicated by other z > 2 galaxies (predominantly quasars; 1525_(-475)~(+1300)). It is unlikely that this rising trend can be accounted for by a contribution of active galactic nucleus (AGN) heating to L_(FIR) alone, and may hint at a higher median gas density and/or elevated star formation efficiency toward the more luminous high-redshift systems. There is marginal evidence that the L_(FIR)/L′_(HCN) ratio in J1148+5251 may even exceed the rising trend set by other z > 2 galaxies; however, only future facilities with very large collecting areas such as the Square Kilometer Array (SKA) will offer the sensitivity required to further investigate this question.
机译:我们报告了使用超大型阵列(VLA)在z = 6.42时对SDSS J114816.64 + 525150.3(以下称J1148 + 5251)的HCN(J = 2→1)发射线进行的灵敏搜索。 HCN的发射是恒星形成的指示剂,它跟踪恒星形成的分子云中的致密分子氢气[n(H_2)≥10〜4 cm〜(-3)]。在J1148 + 5251的深干涉仪图中未检测到发射。我们推导了L'_(HCN)<3.3×10〜9 K km s〜(-1)pc〜2的HCN线亮度极限,对应于L'_(HCN)/ L′_(CO)<0.13。此限制与附近超发光红外星系(ULIRGs)范围内的J1148 + 5251中的高密度分子气体分数一致;中值:L'_(HCN)/ L'_(CO)= 0.17 _(-0.08)〜 (+0.05)和HCN检测到的z> 2个星系(0.17 _(-0.08)〜(+0.09))。L'_(HCN)和L_(FIR)之间的关系被认为是效率的度量在邻近的宇宙中,这些量呈线性相关,因此具有几乎恒定的平均比率,在J1148 + 5251中,我们发现L_(FIR)/ L′_(HCN)> 6600。这远高于正常附近的螺旋星系的平均比率(L_(FIR)/ L'_(HCN)= 580 _(-270)〜(+510)和ULIRG(740 _(-50)〜(+505)) ,但与其他z> 2个星系(主要是类星体; 1525 _(-475)〜(+1300))所指示的上升趋势一致。这种上升趋势不太可能由活动的银河核做出贡献( AGN)仅加热到L_(FIR),并可能暗示更高的气体中位数密度和/或更高的恒星形成效率。有少量证据表明,J1148 + 5251中的L_(FIR)/ L'_(HCN)比甚至可能超过其他z> 2星系设定的上升趋势;但是,只有将来具有非常大的收集面积的设施(例如平方公里阵列(SKA))才能提供进一步研究此问题所需的灵敏度。

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