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arXiv 1808.09243astro-ph.GA
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86 GHz超紧凑河外射电源的全球毫米波VLBI阵列巡天

Global millimeter VLBI array survey of ultracompact extragalactic radio sources at 86 GHz

Dhanya G. Nair, Andrei P. Lobanov, Thomas P. Krichbaum, Eduardo Ros, J. Anton Zensus, Yuri Y. Kovalev, Sang-Sung Lee, Florent Mertens, Yoshiaki Hagiwara, Michae… 展开作者

Dhanya G. Nair, Andrei P. Lobanov, Thomas P. Krichbaum, Eduardo Ros, J. Anton Zensus, Yuri Y. Kovalev, Sang-Sung Lee, Florent Mertens, Yoshiaki Hagiwara, Michael Bremer, Michael Lindqvist, Pablo de Vicente

摘要:

在86 $\,$ GHz(波长,$λ= 3\,$ mm)的甚长基线干涉测量(VLBI)观测达到约50 $μ$ as的分辨率,探测活动星系核中相对论外流的准直和加速区域。为了扩大对致密河外喷流的统计研究,2010-2011年利用全球毫米波VLBI阵列对162个射电源进行了一次大规模的全球86 GHz VLBI调查。测量数据达到了0.1焦耳/束的典型基线灵敏度和5毫焦耳/束的典型图像灵敏度,为所有测量目标提供了成功的探测和图像。对于138个对象,该调查提供了有史以来第一次在86 GHz的VLBI图像。采用高斯模型拟合能见度数据来表征源的结构。高斯模型拟合为基础的估计亮温($T_\mathrm{b}$)在喷流基地(核心)和移动区域(喷流组件)下游的核心进行了比较,估计$T_\mathrm{b}$限制直接从能见度数据,证明了良好的协议之间的两种方法。在我们的样本中,喷流核心的视亮度温度估计值范围从$2.5 \times 10^{9}\,$ K到$ 1.3\times 10^{12}\,$ K。一个人口模型与一个单一的亮度温度,$T_\mathrm{0}$的内在价值,被施加到重现所观察到的$T_\mathrm{b}$分布。它产生$T_\mathrm{0} = (3.77^{+0.10}_{-0.14}) \times 10^{11}\,$ K的射流核心,这意味着逆康普顿损失占主导地位的排放。在喷流分量中,发现$T_\mathrm{0} =(1.42^{+0.16}_{-0.19})\times 10^{11}\,$ K,略高于这些喷流区域预期的$\sim5\times 10^{10}\,$ K的均分极限。对于具有足够结构细节的物体,绝热能量损失占主导地位的观测到的变化$T_\mathrm{b}$沿射流。

英文摘要:

(abridged) Very long baseline interferometry (VLBI) observations at 86$\,$GHz (wavelength, $λ= 3\,$mm) reach a resolution of about 50 $μ$as, probing the collimation and acceleration regions of relativistic outflows in active galactic nuclei. To extend the statistical studies of compact extragalactic jets, a large global 86 GHz VLBI survey of 162 radio sources was conducted in 2010-2011 using the Global Millimeter VLBI Array. The survey data attained a typical baseline sensitivity of 0.1 Jy and a typical image sensitivity of 5 mJy/beam, providing successful detections and images for all of the survey targets. For 138 objects, the survey provides the first ever VLBI images made at 86 GHz. Gaussian model fitting of the visibility data was applied to represent the structure of the sources. The Gaussian model-fit-based estimates of brightness temperature ($T_\mathrm{b}$) at the jet base (core) and in moving regions (jet components) downstream from the core were compared to the estimates of $T_\mathrm{b}$ limits made directly from the visibility data, demonstrating a good agreement between the two methods. The apparent brightness temperature estimates for the jet cores in our sample range from $2.5 \times 10^{9}\,$K to $ 1.3\times 10^{12}\,$K. A population model with a single intrinsic value of brightness temperature, $T_\mathrm{0}$, is applied to reproduce the observed $T_\mathrm{b}$ distribution. It yields $T_\mathrm{0} = (3.77^{+0.10}_{-0.14}) \times 10^{11}\,$K for the jet cores, implying that the inverse Compton losses dominate the emission. In the jet components, $T_\mathrm{0} =(1.42^{+0.16}_{-0.19})\times 10^{11}\,$K is found, slightly higher than the equipartition limit of $\sim5\times 10^{10}\,$K expected for these jet regions. For objects with sufficient structural detail detected, the adiabatic energy losses dominate the observed changes of $T_\mathrm{b}$ along the jet.

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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