利用氨(NH3)(1,1)和(2,2)谱线研究金牛座分子云恒星前核心L1517B中心区域的内部结构

IF 5.4 3区 材料科学 Q2 CHEMISTRY, PHYSICAL
Atanu Koley
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Jansky Very Large Array (VLA) radio telescope (spatial resolution <jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S132335802300053X_inline2.png\" /> <jats:tex-math> $\\sim$ </jats:tex-math> </jats:alternatives> </jats:inline-formula> 3.7<jats:sup>′′</jats:sup>). Our analysis indicates that the central region of the core is close-to-round in shape obtained both from NH<jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S132335802300053X_inline3.png\" /> <jats:tex-math> $_{3}$ </jats:tex-math> </jats:alternatives> </jats:inline-formula> (1,1) and (2,2) emissions. Radially averaged kinetic temperature (<jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S132335802300053X_inline4.png\" /> <jats:tex-math> $T_{k}$ </jats:tex-math> </jats:alternatives> </jats:inline-formula>) is almost constant with a mean value of <jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S132335802300053X_inline5.png\" /> <jats:tex-math> $\\sim$ </jats:tex-math> </jats:alternatives> </jats:inline-formula> 9 K. A radially sharp decrease in kinetic temperature (<jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S132335802300053X_inline6.png\" /> <jats:tex-math> $T_{k}$ </jats:tex-math> </jats:alternatives> </jats:inline-formula>) has not been observed inside the central dense nucleus of this prestellar core. In addition, we also notice that there is an overall velocity gradient from north-east to south-west direction in this region, which may be indicative of the rotational motion of the core. We then calculate the parameter <jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S132335802300053X_inline7.png\" /> <jats:tex-math> $\\beta$ </jats:tex-math> </jats:alternatives> </jats:inline-formula>, which is defined as the ratio of rotational energy to gravitational potential energy and find that <jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S132335802300053X_inline8.png\" /> <jats:tex-math> $\\beta$ </jats:tex-math> </jats:alternatives> </jats:inline-formula> equals to <jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S132335802300053X_inline9.png\" /> <jats:tex-math> $\\sim$ </jats:tex-math> </jats:alternatives> </jats:inline-formula> 5 <jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S132335802300053X_inline10.png\" /> <jats:tex-math> $\\times$ </jats:tex-math> </jats:alternatives> </jats:inline-formula> 10<jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S132335802300053X_inline11.png\" /> <jats:tex-math> $^{-3}$ </jats:tex-math> </jats:alternatives> </jats:inline-formula>; which indicates that rotation has no effect at least inside the central region of the core. We also perform the viral analysis and observe that the central region may be in a stage of contraction. From this study, we also show that turbulence inside the central region is subsonic in nature (sonic Mach number, <jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S132335802300053X_inline12.png\" /> <jats:tex-math> $M_{s}$ </jats:tex-math> </jats:alternatives> </jats:inline-formula><jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S132335802300053X_inline13.png\" /> <jats:tex-math> $&lt;$ </jats:tex-math> </jats:alternatives> </jats:inline-formula> 1) and has no prominent length-scale dependence. Furthermore, we notice that the decrement of excitation temperature (<jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S132335802300053X_inline14.png\" /> <jats:tex-math> $T_{ex}$ </jats:tex-math> </jats:alternatives> </jats:inline-formula>) and column density of NH<jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S132335802300053X_inline15.png\" /> <jats:tex-math> $_{3}$ </jats:tex-math> </jats:alternatives> </jats:inline-formula> from the centre of the core to the outer side with the peak values of <jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S132335802300053X_inline16.png\" /> <jats:tex-math> $\\sim$ </jats:tex-math> </jats:alternatives> </jats:inline-formula> 5.6 K and <jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S132335802300053X_inline17.png\" /> <jats:tex-math> $\\sim$ </jats:tex-math> </jats:alternatives> </jats:inline-formula> 10<jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S132335802300053X_inline18.png\" /> <jats:tex-math> $^{15}$ </jats:tex-math> </jats:alternatives> </jats:inline-formula> cm<jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S132335802300053X_inline19.png\" /> <jats:tex-math> $^{-2}$ </jats:tex-math> </jats:alternatives> </jats:inline-formula>, respectively. In conclusion, this work examines different physical and kinematical properties of the central region of the L1517B prestellar core.","PeriodicalId":4,"journal":{"name":"ACS Applied Energy Materials","volume":null,"pages":null},"PeriodicalIF":5.4000,"publicationDate":"2023-11-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Studying the internal structures of the central region of prestellar core L1517B in Taurus molecular cloud using ammonia (NH3) (1,1) and (2,2) lines\",\"authors\":\"Atanu Koley\",\"doi\":\"10.1017/pasa.2023.53\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Measurement of internal structures in the prestellar core is essential for understanding the initial conditions prior to star formation. In this work, we study the ammonia lines (NH<jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\\\"http://www.w3.org/1999/xlink\\\" mime-subtype=\\\"png\\\" xlink:href=\\\"S132335802300053X_inline1.png\\\" /> <jats:tex-math> $_{3}$ </jats:tex-math> </jats:alternatives> </jats:inline-formula>) (<jats:italic>J</jats:italic>, <jats:italic>K</jats:italic> = 1,1 and 2,2) in the central region of the prestellar core L1517B with the Karl G. Jansky Very Large Array (VLA) radio telescope (spatial resolution <jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\\\"http://www.w3.org/1999/xlink\\\" mime-subtype=\\\"png\\\" xlink:href=\\\"S132335802300053X_inline2.png\\\" /> <jats:tex-math> $\\\\sim$ </jats:tex-math> </jats:alternatives> </jats:inline-formula> 3.7<jats:sup>′′</jats:sup>). Our analysis indicates that the central region of the core is close-to-round in shape obtained both from NH<jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\\\"http://www.w3.org/1999/xlink\\\" mime-subtype=\\\"png\\\" xlink:href=\\\"S132335802300053X_inline3.png\\\" /> <jats:tex-math> $_{3}$ </jats:tex-math> </jats:alternatives> </jats:inline-formula> (1,1) and (2,2) emissions. Radially averaged kinetic temperature (<jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\\\"http://www.w3.org/1999/xlink\\\" mime-subtype=\\\"png\\\" xlink:href=\\\"S132335802300053X_inline4.png\\\" /> <jats:tex-math> $T_{k}$ </jats:tex-math> </jats:alternatives> </jats:inline-formula>) is almost constant with a mean value of <jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\\\"http://www.w3.org/1999/xlink\\\" mime-subtype=\\\"png\\\" xlink:href=\\\"S132335802300053X_inline5.png\\\" /> <jats:tex-math> $\\\\sim$ </jats:tex-math> </jats:alternatives> </jats:inline-formula> 9 K. A radially sharp decrease in kinetic temperature (<jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\\\"http://www.w3.org/1999/xlink\\\" mime-subtype=\\\"png\\\" xlink:href=\\\"S132335802300053X_inline6.png\\\" /> <jats:tex-math> $T_{k}$ </jats:tex-math> </jats:alternatives> </jats:inline-formula>) has not been observed inside the central dense nucleus of this prestellar core. In addition, we also notice that there is an overall velocity gradient from north-east to south-west direction in this region, which may be indicative of the rotational motion of the core. We then calculate the parameter <jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\\\"http://www.w3.org/1999/xlink\\\" mime-subtype=\\\"png\\\" xlink:href=\\\"S132335802300053X_inline7.png\\\" /> <jats:tex-math> $\\\\beta$ </jats:tex-math> </jats:alternatives> </jats:inline-formula>, which is defined as the ratio of rotational energy to gravitational potential energy and find that <jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\\\"http://www.w3.org/1999/xlink\\\" mime-subtype=\\\"png\\\" xlink:href=\\\"S132335802300053X_inline8.png\\\" /> <jats:tex-math> $\\\\beta$ </jats:tex-math> </jats:alternatives> </jats:inline-formula> equals to <jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\\\"http://www.w3.org/1999/xlink\\\" mime-subtype=\\\"png\\\" xlink:href=\\\"S132335802300053X_inline9.png\\\" /> <jats:tex-math> $\\\\sim$ </jats:tex-math> </jats:alternatives> </jats:inline-formula> 5 <jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\\\"http://www.w3.org/1999/xlink\\\" mime-subtype=\\\"png\\\" xlink:href=\\\"S132335802300053X_inline10.png\\\" /> <jats:tex-math> $\\\\times$ </jats:tex-math> </jats:alternatives> </jats:inline-formula> 10<jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\\\"http://www.w3.org/1999/xlink\\\" mime-subtype=\\\"png\\\" xlink:href=\\\"S132335802300053X_inline11.png\\\" /> <jats:tex-math> $^{-3}$ </jats:tex-math> </jats:alternatives> </jats:inline-formula>; which indicates that rotation has no effect at least inside the central region of the core. We also perform the viral analysis and observe that the central region may be in a stage of contraction. From this study, we also show that turbulence inside the central region is subsonic in nature (sonic Mach number, <jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\\\"http://www.w3.org/1999/xlink\\\" mime-subtype=\\\"png\\\" xlink:href=\\\"S132335802300053X_inline12.png\\\" /> <jats:tex-math> $M_{s}$ </jats:tex-math> </jats:alternatives> </jats:inline-formula><jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\\\"http://www.w3.org/1999/xlink\\\" mime-subtype=\\\"png\\\" xlink:href=\\\"S132335802300053X_inline13.png\\\" /> <jats:tex-math> $&lt;$ </jats:tex-math> </jats:alternatives> </jats:inline-formula> 1) and has no prominent length-scale dependence. Furthermore, we notice that the decrement of excitation temperature (<jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\\\"http://www.w3.org/1999/xlink\\\" mime-subtype=\\\"png\\\" xlink:href=\\\"S132335802300053X_inline14.png\\\" /> <jats:tex-math> $T_{ex}$ </jats:tex-math> </jats:alternatives> </jats:inline-formula>) and column density of NH<jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\\\"http://www.w3.org/1999/xlink\\\" mime-subtype=\\\"png\\\" xlink:href=\\\"S132335802300053X_inline15.png\\\" /> <jats:tex-math> $_{3}$ </jats:tex-math> </jats:alternatives> </jats:inline-formula> from the centre of the core to the outer side with the peak values of <jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\\\"http://www.w3.org/1999/xlink\\\" mime-subtype=\\\"png\\\" xlink:href=\\\"S132335802300053X_inline16.png\\\" /> <jats:tex-math> $\\\\sim$ </jats:tex-math> </jats:alternatives> </jats:inline-formula> 5.6 K and <jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\\\"http://www.w3.org/1999/xlink\\\" mime-subtype=\\\"png\\\" xlink:href=\\\"S132335802300053X_inline17.png\\\" /> <jats:tex-math> $\\\\sim$ </jats:tex-math> </jats:alternatives> </jats:inline-formula> 10<jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\\\"http://www.w3.org/1999/xlink\\\" mime-subtype=\\\"png\\\" xlink:href=\\\"S132335802300053X_inline18.png\\\" /> <jats:tex-math> $^{15}$ </jats:tex-math> </jats:alternatives> </jats:inline-formula> cm<jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\\\"http://www.w3.org/1999/xlink\\\" mime-subtype=\\\"png\\\" xlink:href=\\\"S132335802300053X_inline19.png\\\" /> <jats:tex-math> $^{-2}$ </jats:tex-math> </jats:alternatives> </jats:inline-formula>, respectively. In conclusion, this work examines different physical and kinematical properties of the central region of the L1517B prestellar core.\",\"PeriodicalId\":4,\"journal\":{\"name\":\"ACS Applied Energy Materials\",\"volume\":null,\"pages\":null},\"PeriodicalIF\":5.4000,\"publicationDate\":\"2023-11-16\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"ACS Applied Energy Materials\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://doi.org/10.1017/pasa.2023.53\",\"RegionNum\":3,\"RegionCategory\":\"材料科学\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"CHEMISTRY, PHYSICAL\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"ACS Applied Energy Materials","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.1017/pasa.2023.53","RegionNum":3,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"CHEMISTRY, PHYSICAL","Score":null,"Total":0}
引用次数: 0

摘要

对恒星前核心内部结构的测量对于理解恒星形成前的初始条件至关重要。在这项工作中,我们使用Karl G. Jansky甚大阵列(VLA)射电望远镜(空间分辨率$\sim$ 3.7”)研究了恒星前核心L1517B中心区域的氨谱线(NH $_{3}$) (J, K = 1,1和2,2)。我们的分析表明,从NH $_{3}$(1,1)和(2,2)发射中获得的核心中心区域的形状接近圆形。径向平均动力学温度($T_{k}$)几乎是恒定的,平均值为$\sim$ 9k。在这个恒星前核心的中心致密核内,没有观察到动力学温度的径向急剧下降($T_{k}$)。此外,我们还注意到该区域整体速度梯度从东北向西南方向,这可能表明了地核的旋转运动。然后计算参数$\beta$,定义为旋转能与重力势能之比,得到$\beta$ = $\sim$ 5 $\times$ 10 $^{-3}$;这表明旋转至少在地核的中心区域内没有影响。我们还进行了病毒分析,观察到中心区域可能处于收缩阶段。从这项研究中,我们还表明,中心区域内的湍流本质上是亚音速的(音速马赫数,$M_{s}$$<$ 1),并且没有明显的长度尺度依赖性。此外,我们注意到激发温度($T_{ex}$)和NH柱密度$_{3}$从核心中心向外侧递减,峰值分别为$\sim$ 5.6 K和$\sim$ 10 $^{15}$ cm $^{-2}$。总之,这项工作考察了L1517B恒星前核心中心区域的不同物理和运动学特性。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Studying the internal structures of the central region of prestellar core L1517B in Taurus molecular cloud using ammonia (NH3) (1,1) and (2,2) lines
Measurement of internal structures in the prestellar core is essential for understanding the initial conditions prior to star formation. In this work, we study the ammonia lines (NH $_{3}$ ) (J, K = 1,1 and 2,2) in the central region of the prestellar core L1517B with the Karl G. Jansky Very Large Array (VLA) radio telescope (spatial resolution $\sim$ 3.7′′). Our analysis indicates that the central region of the core is close-to-round in shape obtained both from NH $_{3}$ (1,1) and (2,2) emissions. Radially averaged kinetic temperature ( $T_{k}$ ) is almost constant with a mean value of $\sim$ 9 K. A radially sharp decrease in kinetic temperature ( $T_{k}$ ) has not been observed inside the central dense nucleus of this prestellar core. In addition, we also notice that there is an overall velocity gradient from north-east to south-west direction in this region, which may be indicative of the rotational motion of the core. We then calculate the parameter $\beta$ , which is defined as the ratio of rotational energy to gravitational potential energy and find that $\beta$ equals to $\sim$ 5 $\times$ 10 $^{-3}$ ; which indicates that rotation has no effect at least inside the central region of the core. We also perform the viral analysis and observe that the central region may be in a stage of contraction. From this study, we also show that turbulence inside the central region is subsonic in nature (sonic Mach number, $M_{s}$ $<$ 1) and has no prominent length-scale dependence. Furthermore, we notice that the decrement of excitation temperature ( $T_{ex}$ ) and column density of NH $_{3}$ from the centre of the core to the outer side with the peak values of $\sim$ 5.6 K and $\sim$ 10 $^{15}$ cm $^{-2}$ , respectively. In conclusion, this work examines different physical and kinematical properties of the central region of the L1517B prestellar core.
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来源期刊
ACS Applied Energy Materials
ACS Applied Energy Materials Materials Science-Materials Chemistry
CiteScore
10.30
自引率
6.20%
发文量
1368
期刊介绍: ACS Applied Energy Materials is an interdisciplinary journal publishing original research covering all aspects of materials, engineering, chemistry, physics and biology relevant to energy conversion and storage. The journal is devoted to reports of new and original experimental and theoretical research of an applied nature that integrate knowledge in the areas of materials, engineering, physics, bioscience, and chemistry into important energy applications.
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