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2
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Astron Astrophys. 2018 Feb;610. doi: 10.1051/0004-6361/201731619. Epub 2018 Feb 7.
3
The growth of carbon chains in IRC +10216 mapped with ALMA.用阿塔卡马大型毫米/亚毫米波阵列(ALMA)绘制的IRC +10216中碳链的生长情况。
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4
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5
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6
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7
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8
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10
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IRC+10216中SIS谱线(J=14-13和15-14)的脉泽发射结构与时间变化

The Maser Emitting Structure and Time Variability of the SIS Lines = 14 - 13 and 15 - 14 in IRC+10216.

作者信息

Fonfría J P, Fernández-López M, Pardo J R, Agúndez M, Sánchez Contreras C, Velilla Prieto L, Cernicharo J, Santander-García M, Quintana-Lacaci G, Castro-Carrizo A, Curiel S

机构信息

Molecular Astrophysics Group, Instituto de Ciencia de Materiales de Madrid, CSIC, C/ Sor Juana Inés de la Cruz, 3, Cantoblanco, 28049, Madrid (Spain).

Molecular Astrophysics Group, Instituto de Física Fundamental, CSIC, C/ Serrano, 123, 28006, Madrid (Spain).

出版信息

Astrophys J. 2018 Jun 20;860(2). doi: 10.3847/1538-4357/aac5e3.

DOI:10.3847/1538-4357/aac5e3
PMID:29977091
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC6029660/
Abstract

We present new high angular resolution interferometer observations of the = 0 = 14 - 13 and 15 - 14 SiS lines towards IRC+10216, carried out with CARMA and ALMA. The maps, with angular resolutions of reveal (1) an extended, roughly uniform, and weak emission with a size of (2) a component elongated approximately along the East-West direction peaking at at both sides of the central star, and (3) two blue- and red-shifted compact components peaking around to the NW of the star. We have modeled the emission with a 3D radiation transfer code finding that the observations cannot be explained only by thermal emission. Several maser clumps and one arc-shaped maser feature arranged from 5 to 20 from the central star, in addition to a thin shell-like maser structure at ≃ 13 are required to explain the observations. This maser emitting set of structures accounts for 75% of the total emission while the other 25% is produced by thermally excited molecules. About 60% of the maser emission comes from the extended emission and the rest from the set of clumps and the arc. The analysis of a time monitoring of these and other SiS and SiS lines carried out with the IRAM 30 m telescope from 2015 to present suggests that the intensity of some spectral components of the maser emission strongly depends on the stellar pulsation while other components show a mild variability. This monitoring evidences a significant phase lag of ≃ 0.2 between the maser and NIR light-curves.

摘要

我们展示了使用卡尔玛(CARMA)和阿塔卡马大型毫米波阵(ALMA)对IRC+10216方向的J = 0、K = 14 - 13和15 - 14的SiS谱线进行的新高角分辨率干涉测量观测结果。这些角分辨率为[具体分辨率数值未给出]的地图显示:(1)存在一个扩展的、大致均匀且微弱的发射区域,大小为[具体大小数值未给出];(2)一个大致沿东西方向拉长的分量,在中央恒星两侧峰值位于[具体位置数值未给出];(3)两个蓝移和红移的致密分量,在恒星西北方向峰值位于[具体位置数值未给出]。我们使用三维辐射传输代码对发射进行了建模,发现观测结果不能仅用热发射来解释。除了在≃13处的薄壳状脉泽结构外,还需要几个脉泽团块和一个从中央恒星向外5到20处排列的弧形脉泽特征来解释观测结果。这套脉泽发射结构占总发射的75%,而另外25%由热激发分子产生。约60%的脉泽发射来自扩展发射,其余来自团块和弧形结构。对2015年至今使用IRAM 30米望远镜对这些以及其他SiS和SiS谱线进行的时间监测分析表明,脉泽发射的一些光谱分量的强度强烈依赖于恒星脉动,而其他分量显示出轻微变化。该监测证明脉泽和近红外光变曲线之间存在约0.2的显著相位滞后。

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