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AzTEC/ASTE对AKARI深野外南部的1.1毫米测量:震源目录和数量计数

AzTEC/ASTE 1.1-mm Survey of the AKARI Deep Field South: source catalogue and number counts

B. Hatsukade, K. Kohno, I. Aretxaga, J. E. Austermann, H. Ezawa, D. H. Hughes, S. Ikarashi, D. Iono, R. Kawabe, S. Khan, H. Matsuo, S. Matsuura, K. Nakanishi, T… 展开作者

B. Hatsukade, K. Kohno, I. Aretxaga, J. E. Austermann, H. Ezawa, D. H. Hughes, S. Ikarashi, D. Iono, R. Kawabe, S. Khan, H. Matsuo, S. Matsuura, K. Nakanishi, T. Oshima, T. Perera, K. S. Scott, M. Shirahata, T. T. Takeuchi, Y. Tamura, K. Tanaka, T. Tosaki, G. W. Wilson, M. S. Yun

摘要:

我们目前的AKARI深场南(ADF-S)与AzTEC安装在阿塔卡马亚毫米望远镜实验(ASTE)的1.1毫米深的调查结果。我们得到了0.25平方米的地图。deg区域,均方根噪声电平为0.32-0.71 mJy。这是迄今为止在毫米和亚毫米波长上最深和最宽的地图之一。我们发现了198个显著性为3.5-15.6 sigma的源,提供了相邻区域中最大的1.1 mm源目录。大多数辐射源在AKARI卫星的远红外波段都没有被探测到,这表明它们大多位于z ~ 1.5的探测极限。我们在ADF-S,斯巴鲁/XMM牛顿深场(SXDF)和AzTEC/ASTE调查的SSA 22场中构建了差分和累积计数,这些场提供了目前对微弱端的最严格限制。ADF-S中最佳拟合计数的积分发现,通量>=1 mJy的1.1 mm源对1.1 mm处宇宙红外背景(CIB)的贡献为12- 16%,这表明大部分CIB来自数量计数尚未受到约束的微弱源。我们使用ADF-S中的最佳拟合数计数估计了大于等于1 mJy的1.1 mm源所贡献的宇宙恒星形成率密度,发现它比来自z ~ 2-3的UV/光学选择星系的宇宙恒星形成率密度低约5-10倍。通过恒星形成速率密度的时间积分计算,在z >= 1时,1.1 mm源产生的大于1 mJy的恒星质量在现今宇宙中所占的比例约为20%。如果我们考虑再循环分数>0.4,这是形成恒星的物质返回到星际介质的分数,由1.1 mm源产生的恒星质量的分数下降到<~ 10%。

英文摘要:

We present results of a 1.1 mm deep survey of the AKARI Deep Field South (ADF-S) with AzTEC mounted on the Atacama Submillimetre Telescope Experiment (ASTE). We obtained a map of 0.25 sq. deg area with an rms noise level of 0.32-0.71 mJy. This is one of the deepest and widest maps thus far at millimetre and submillimetre wavelengths. We uncovered 198 sources with a significance of 3.5-15.6 sigma, providing the largest catalog of 1.1 mm sources in a contiguous region. Most of the sources are not detected in the far-infrared bands of the AKARI satellite, suggesting that they are mostly at z ~ 1.5 given the detection limits. We constructed differential and cumulative number counts in the ADF-S, the Subaru/XMM Newton Deep Field (SXDF), and the SSA 22 field surveyed by AzTEC/ASTE, which provide currently the tightest constraints on the faint end. The integration of the best-fit number counts in the ADF-S find that the contribution of 1.1 mm sources with fluxes >=1 mJy to the cosmic infrared background (CIB) at 1.1 mm is 12-16%, suggesting that the large fraction of the CIB originates from faint sources of which the number counts are not yet constrained. We estimate the cosmic star-formation rate density contributed by 1.1 mm sources with >=1 mJy using the best-fit number counts in the ADF-S and find that it is lower by about a factor of 5-10 compared to those derived from UV/optically-selected galaxies at z ~ 2-3. The fraction of stellar mass of the present-day universe produced by 1.1 mm sources with >=1 mJy at z >= 1 is ~20%, calculated by the time integration of the star-formation rate density. If we consider the recycled fraction of >0.4, which is the fraction of materials forming stars returned to the interstellar medium, the fraction of stellar mass produced by 1.1 mm sources decrease to <~10%.

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