{"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> $<$ </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}
引用次数: 0
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 $_{3}$ ) (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.
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.