Pub Date : 2024-07-23DOI: 10.1051/0004-6361/202349136
N. Duronea, L. Bronfman, M. Ortega, L. Suad, G. Baume, E. Mendoza, M. Carvajal, S. Cichowolski, E. M. Arnal, R. Finger, M. Merello, R. Gamen
In this paper, we present a new multifrequency study of the giant star-forming complex RCW,122. We used molecular data obtained with the ASTE 10 m and the APEX 12 m telescopes, along with infrared observations spanning from 3.6 to 870 obtained from available databases. We also incorporated a range of public datasets, including the radio continuum at 3 GHz, narrowband Halpha images, and deep JHK photometry. Our analysis focuses mostly on cataloged ATLASGAL sources, showcasing a spectrum of evolutionary stages from infrared dark cloud (IRDC)/high-mass protostellar object (HMPO) to ultra-compact HII region (UCHII), as inferred from preliminary inspections of the public dataset. Based on ASTE HCO$^+$(4--3) and CO(3--2) data, we identified five molecular clumps, designated A, B, C, D, and E, as molecular counterparts of the ATLASGAL sources. These clumps have radial velocities ranging from sim --15 to --10 confirming their association with RCW,122. In addition, we report the detection of 20 transitions from 11 distinct molecules in the APEX spectra in the frequency ranges from 228.538 GHz to 232.538 GHz and 218.3 to 222.3 GHz, unveiling a diverse chemical complexity among the clumps. Utilizing CO(2--1) and C18O(2--1) data taken from the observations with the APEX telescope we estimated the total LTE molecular mass, ranging from 200 $M_ odot $ (clump A) to 4400 $M_ odot $ (clump B). Our mid- to far-infrared (MIR-FIR) flux density analysis yielded minimum dust temperatures of 23.7 K (clump A) to maximum temperatures of 33.9 K (clump B), indicating varying degrees of internal heating among the clumps. The bolometric luminosities span 1.7times 10$^3$ L$_ odot $ (clump A) to 2.4times 10$^5$ L$_ odot $ (clump B), while the total (dust+gas) mass ranges from 350 $M_ odot $ (clump A) to 3800 $M_ odot $ (clump B). Our analysis of the molecular line richness, $L/M$ ratios, and CH$_3$CCH and dust temperatures reveals an evolutionary sequence of A/Erightarrow Crightarrow D/B, consistent with preliminary inferences of the ATLASGAL sources. In this context, clumps A and E exhibit early stages of collapse, with clump A likely in an early HMPO phase, which is supported by identifying a candidate molecular outflow. Clump E appears to be in an intermediate stage between IRDC and HMPO. Clumps D and B show evidence of being in the UCHII phase, with clump B likely more advanced. Clump C likely represents an intermediate stage between HMPO and HMC. Our findings suggest clump B is undergoing ionization and heating by multiple stellar and protostellar members of the stellar cluster DBS,119. Meanwhile, other cluster members may be responsible for ionizing other regions of RCW,122 that have evolved into fully developed HII regions, beyond the molecular dissociation stage.
在本文中,我们对巨型恒星形成复合体 RCW,122 进行了一项新的多频研究。我们使用了 ASTE 10 m 和 APEX 12 m 望远镜获得的分子数据,以及从现有数据库中获得的从 3.6 到 870 波段的红外观测数据。我们还纳入了一系列公共数据集,包括 3 GHz 的射电连续波、窄带 Halpha 图像和深度 JHK 测光。我们的分析主要集中在编录的ATLASGAL源上,展示了从红外暗云(IRDC)/高质原恒星天体(HMPO)到超小型HII区(UCHII)等演化阶段的光谱,这是从对公共数据集的初步检查中推断出来的。根据ASTE HCO$^+$(4--3)和CO(3--2)数据,我们确定了五个分子团块,分别命名为A、B、C、D和E,作为ATLASGAL源的分子对应物。这些分子团块的径向速度从sim --15 到 --10,证实了它们与RCW,122的联系。此外,我们还报告说在APEX光谱的228.538 GHz到232.538 GHz和218.3到222.3 GHz频率范围内探测到了来自11种不同分子的20次跃迁,揭示了星团中复杂多样的化学成分。利用 APEX 望远镜观测到的 CO(2--1) 和 C18O(2--1) 数据,我们估算出了 LTE 的总分子质量,范围从 200M_ odot $(星团 A)到 4400M_ odot $(星团 B)。我们的中远红外(MIR-FIR)通量密度分析得出尘埃的最低温度为 23.7 K(星团 A),最高温度为 33.9 K(星团 B),这表明星团之间存在不同程度的内部加热。测光度从 1.7times 10$^3$ L$_ odot $(星团 A)到 2.4times 10$^5$ L$_ odot $(星团 B)不等,而总质量(尘埃+气体)从 350 $M_ odot $(星团 A)到 3800 $M_ odot $(星团 B)不等。我们对分子线丰富度、$L/M$比值、CH$_3$CCH和尘埃温度的分析表明,A/Erightarrow Crightarrow D/B的演化序列与ATLASGAL源的初步推断一致。在这种情况下,星团 A 和 E 显示出坍缩的早期阶段,星团 A 很可能处于早期 HMPO 阶段,这一点可以通过识别候选分子外流得到支持。星团 E 似乎处于 IRDC 和 HMPO 之间的中间阶段。星团 D 和 B 显示出处于 UCHII 阶段的迹象,其中星团 B 可能更晚些。团块 C 可能处于 HMPO 和 HMC 之间的中间阶段。我们的研究结果表明,星团DBS,119的多个恒星和原恒星成员正在对星团B进行电离和加热。同时,星团的其他成员也可能负责电离 RCW,122 的其他区域,这些区域已经演化成发育完全的 HII 区域,超过了分子解离阶段。
{"title":"Revisiting the massive star-forming complex RCW 122: New millimeter and submillimeter study","authors":"N. Duronea, L. Bronfman, M. Ortega, L. Suad, G. Baume, E. Mendoza, M. Carvajal, S. Cichowolski, E. M. Arnal, R. Finger, M. Merello, R. Gamen","doi":"10.1051/0004-6361/202349136","DOIUrl":"https://doi.org/10.1051/0004-6361/202349136","url":null,"abstract":"In this paper, we present a new multifrequency study of the giant star-forming complex RCW,122. We used molecular data obtained with the ASTE 10 m and the APEX 12 m telescopes, along with infrared observations spanning from 3.6 to 870 obtained from available databases. We also incorporated a range of public datasets, including the radio continuum at 3 GHz, narrowband Halpha images, and deep JHK photometry. Our analysis focuses mostly on cataloged ATLASGAL sources, showcasing a spectrum of evolutionary stages from infrared dark cloud (IRDC)/high-mass protostellar object (HMPO) to ultra-compact HII region (UCHII), as inferred from preliminary inspections of the public dataset. Based on ASTE HCO$^+$(4--3) and CO(3--2) data, we identified five molecular clumps, designated A, B, C, D, and E, as molecular counterparts of the ATLASGAL sources. These clumps have radial velocities ranging from sim --15 to --10 confirming their association with RCW,122. In addition, we report the detection of 20 transitions from 11 distinct molecules in the APEX spectra in the frequency ranges from 228.538 GHz to 232.538 GHz and 218.3 to 222.3 GHz, unveiling a diverse chemical complexity among the clumps. Utilizing CO(2--1) and C18O(2--1) data taken from the observations with the APEX telescope we estimated the total LTE molecular mass, ranging from 200 $M_ odot $ (clump A) to 4400 $M_ odot $ (clump B). Our mid- to far-infrared (MIR-FIR) flux density analysis yielded minimum dust temperatures of 23.7 K (clump A) to maximum temperatures of 33.9 K (clump B), indicating varying degrees of internal heating among the clumps. The bolometric luminosities span 1.7times 10$^3$ L$_ odot $ (clump A) to 2.4times 10$^5$ L$_ odot $ (clump B), while the total (dust+gas) mass ranges from 350 $M_ odot $ (clump A) to 3800 $M_ odot $ (clump B). Our analysis of the molecular line richness, $L/M$ ratios, and CH$_3$CCH and dust temperatures reveals an evolutionary sequence of A/Erightarrow Crightarrow D/B, consistent with preliminary inferences of the ATLASGAL sources. In this context, clumps A and E exhibit early stages of collapse, with clump A likely in an early HMPO phase, which is supported by identifying a candidate molecular outflow. Clump E appears to be in an intermediate stage between IRDC and HMPO. Clumps D and B show evidence of being in the UCHII phase, with clump B likely more advanced. Clump C likely represents an intermediate stage between HMPO and HMC. Our findings suggest clump B is undergoing ionization and heating by multiple stellar and protostellar members of the stellar cluster DBS,119. Meanwhile, other cluster members may be responsible for ionizing other regions of RCW,122 that have evolved into fully developed HII regions, beyond the molecular dissociation stage.","PeriodicalId":8585,"journal":{"name":"Astronomy & Astrophysics","volume":"119 3","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-07-23","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141812000","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-07-23DOI: 10.1051/0004-6361/202348726
Lucas M. Jordan, Dennis Wehner, Rolf Kuiper
Previous simulations of cataclysmic variables studied either the quiescence, or the outburst state in multiple dimensions or they simulated complete outburst cycles in one dimension using simplified models for the gravitational torques. We self-consistently simulate complete outburst cycles of normal and superoutbursts in cataclysmic variable systems in two dimensions. We study the effect of different alpha viscosity parameters, mass transfer rates, and binary mass ratios on the disk luminosities, outburst occurrence rates, and superhumps. We simulate non-isothermal, viscous accretion disks in cataclysmic variable systems using a modified version of the Fargo code with an updated equation of state and a cooling function designed to reproduce s-curve behavior. Our simulations can model complete outburst cycles using the thermal tidal instability model. We find higher superhump amplitudes and stronger gravitational torques than previous studies, resulting in better agreement with observations.
以前对大爆发变星的模拟研究要么是静止状态,要么是多维度的爆发状态,要么是利用引力力矩的简化模型在一维中模拟完整的爆发周期。我们在两个维度上自洽地模拟了大爆发变星系统中正常爆发和超级爆发的完整爆发周期。我们研究了不同的阿尔法粘度参数、质量转移率和双星质量比对磁盘光度、爆发发生率和超暴发的影响。我们使用改进版的 Fargo 代码模拟了大爆发变星系统中的非等温粘性吸积盘,并更新了状态方程和冷却函数,以重现 s 曲线行为。我们的模拟可以利用热潮汐不稳定性模型来模拟完整的爆发周期。与之前的研究相比,我们发现了更高的超冲振幅和更强的引力扭矩,从而与观测结果更加吻合。
{"title":"Two-dimensional simulations of disks in close binaries. Simulating outburst cycles in cataclysmic variables","authors":"Lucas M. Jordan, Dennis Wehner, Rolf Kuiper","doi":"10.1051/0004-6361/202348726","DOIUrl":"https://doi.org/10.1051/0004-6361/202348726","url":null,"abstract":"Previous simulations of cataclysmic variables studied either the\u0000 quiescence, or the outburst state in multiple dimensions or they simulated complete outburst cycles\u0000 in one dimension using simplified models for the gravitational torques. We self-consistently simulate complete outburst cycles\u0000 of normal and superoutbursts in cataclysmic variable systems in two dimensions.\u0000 We study the effect of different alpha viscosity parameters, mass transfer rates,\u0000 and binary mass ratios on the disk luminosities, outburst occurrence rates, and superhumps. We simulate non-isothermal, viscous accretion disks in cataclysmic variable systems\u0000 using a modified version of the Fargo code with an updated equation of state\u0000 and a cooling function designed to reproduce s-curve behavior. Our simulations can model complete outburst cycles\u0000 using the thermal tidal instability model.\u0000 We find higher superhump amplitudes and stronger gravitational torques \u0000 than previous studies, resulting in better agreement with observations.","PeriodicalId":8585,"journal":{"name":"Astronomy & Astrophysics","volume":"53 2","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-07-23","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141810463","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-07-23DOI: 10.1051/0004-6361/202449529
P. Molaro, P. Bonifacio, G. Cupani, J. C. Howk
The line of sight toward Sk 143 (AzV 456), an O9.5 Ib star in the Small Magellanic Cloud (SMC), shows significant absorption from neutral atoms and molecules. We report a new study of this line of sight by means of high-resolution spectra obtained with the ESPRESSO spectrograph at the VLT of ESO. The absorption from neutral and ionized species is well characterized by a single component at v$_ hel $ approx +132 that was modeled with the ASTROCOOK code. The rubidium Rb I 780.0 nm line is detected for the first time outside the Galaxy, and we derive Rb/H = -1.86 pm 0.09. As a result of the high resolution, the 85Rb and 87Rb isotope lines are also exceptionally well resolved. The 85Rb/87Rb isotope ratio is 0.46, which is opposite of the meteoritic value of 2.43. This implies that Rb is made through a dominant contribution of the $r$-process, which is dominant for the 87Rb isotope. We also confirm the presence of 670.7 nm and set a limit on the isotopic ratio of $^6$Li/$^7Li$ < 0.1. The dominance of the 87Rb isotope implies that Rb is made through a dominant contribution of the $r$-process. At the low metallicity of the cloud of Zn/H = -1.28 pm 0.09 , neutron rich material may have occurred in rotating metal-poor massive stars. Moreover, the low metallicity of the cloud leads to an absolute Li abundance of A($^7$Li) approx 2.2, which differs from the expectation from big bang nucleosynthesis. Because the gas-phase abundance is not affected by stellar depletion, the burning of Li inside the halo stars is probably not the solution for the cosmological $^7$Li problem.
{"title":"Extragalactic 85Rb/87Rb and 6Li/ ^7Li ratios in the Small Magellanic Cloud","authors":"P. Molaro, P. Bonifacio, G. Cupani, J. C. Howk","doi":"10.1051/0004-6361/202449529","DOIUrl":"https://doi.org/10.1051/0004-6361/202449529","url":null,"abstract":"The line of sight toward Sk 143 (AzV 456), an O9.5 Ib star in the Small Magellanic Cloud (SMC), shows significant\u0000absorption from neutral atoms and molecules. We report a new study of this line of sight by means of high-resolution spectra obtained with the ESPRESSO spectrograph at the VLT of ESO. The absorption from neutral and ionized species is well characterized by a single component at v$_ hel $ approx +132 that was modeled with the ASTROCOOK code. The \u0000 rubidium Rb I 780.0 nm line is detected for the first time outside the Galaxy, and we derive Rb/H = -1.86 pm 0.09. As a result of the high resolution, the 85Rb and 87Rb isotope lines are also exceptionally well resolved. The 85Rb/87Rb isotope ratio is 0.46, which\u0000 is opposite of the meteoritic value of 2.43. \u0000 This implies that Rb is made through a dominant contribution of the $r$-process, which is dominant for the 87Rb isotope. We also confirm the presence of 670.7 nm and set a limit on the isotopic ratio of $^6$Li/$^7Li$ < 0.1. The dominance of the 87Rb isotope implies that Rb is made through a dominant contribution of the $r$-process. At the low metallicity of the cloud of Zn/H = -1.28 pm 0.09 , neutron rich material may have occurred in rotating metal-poor massive stars. Moreover, the\u0000 low metallicity of the cloud leads to an absolute Li abundance of A($^7$Li) approx 2.2, which differs from the expectation from big bang nucleosynthesis. Because the gas-phase abundance is not affected by stellar depletion, the burning of Li inside the halo stars is probably not the solution for the cosmological $^7$Li problem.","PeriodicalId":8585,"journal":{"name":"Astronomy & Astrophysics","volume":"141 7","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-07-23","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141811135","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-07-22DOI: 10.1051/0004-6361/202450606
V. Wakelam, P. Gratier, J. Loison, K. M. Hickson, J. Penguen, A. Mechineau
The study of the chemical composition of the interstellar medium (ISM) requires a strong synergy between laboratory astrophysics, modeling, and observations. In particular, astrochemical models have been developed for decades now and include an increasing number of processes studied in the laboratory or theoretically. These models follow the chemistry both in the gas phase and at the surface of interstellar grains. Since 2012, we have provided complete gas-phase chemical networks for astrochemical codes that can be used to model various environments of the ISM. Our aim is to introduce the new up-to-date astrochemical network kida.uva.2024 together with the ice chemical network and the fortran code to compute time dependent compositions of the gas, the ice surface, and the ice mantles under physical conditions relevant for the ISM. The gas-phase chemical reactions, as well as associated rate coefficients, included in kida.uva.2024 were carefully selected from the KIDA online database and represent the most recent values. The model predictions for cold core conditions and for when considering only gas-phase processes were computed as a function of time and compared to the predictions obtained with the previous version, kida.uva.2014. In addition, key chemical reactions were identified. The model predictions, including both gas and surface processes, were compared to the molecular abundances as observed in the cold core TMC1-CP. Many gas-phase reactions were revised or added to produce kida.uva.2024. The new model predictions are different by several orders of magnitude for some species. The agreement of this new model with observations in TMC-1 (CP) is, however, similar to the one obtained with the previous network.
研究星际介质(ISM)的化学成分需要实验室天体物理学、建模和观测之间的强大协同作用。特别是,天体化学模型已经发展了几十年,包括越来越多的实验室或理论研究过程。这些模型跟踪气相和星际颗粒表面的化学过程。自 2012 年以来,我们为天体化学代码提供了完整的气相化学网络,可用于模拟 ISM 的各种环境。我们的目的是介绍最新的天体化学网络kida.uva.2024以及冰化学网络和fortran代码,以计算ISM相关物理条件下与时间相关的气体、冰表面和冰幔成分。kida.uva.2024中包含的气相化学反应以及相关速率系数是从KIDA在线数据库中精心挑选的,代表了最新的数值。计算了冷核条件下和仅考虑气相过程时的模型预测值与时间的函数关系,并与前一版本(kida.uva.2014)的预测值进行了比较。此外,还确定了关键的化学反应。包括气相和表面过程在内的模型预测结果与在冷核 TMC1-CP 中观测到的分子丰度进行了比较。对许多气相反应进行了修订或添加,以生成 kida.uva.2024。新模型对某些物种的预测相差几个数量级。然而,这个新模型与在 TMC-1(CP)中观测到的结果的吻合程度与先前网络得到的结果相似。
{"title":"The 2024 KIDA network for interstellar chemistry","authors":"V. Wakelam, P. Gratier, J. Loison, K. M. Hickson, J. Penguen, A. Mechineau","doi":"10.1051/0004-6361/202450606","DOIUrl":"https://doi.org/10.1051/0004-6361/202450606","url":null,"abstract":"The study of the chemical composition of the interstellar medium (ISM) requires a strong synergy between laboratory astrophysics, modeling, and observations. In particular, astrochemical models have been developed for decades now and include an increasing number of processes studied in the laboratory or theoretically. These models follow the chemistry both in the gas phase and at the surface of interstellar grains. Since 2012, we have provided complete gas-phase chemical networks for astrochemical codes that can be used to model various environments of the ISM. Our aim is to introduce the new up-to-date astrochemical network kida.uva.2024 together with the ice chemical network and the fortran code to compute time dependent compositions of the gas, the ice surface, and the ice mantles under physical conditions relevant for the ISM. The gas-phase chemical reactions, as well as associated rate coefficients, included in kida.uva.2024 were carefully selected from the KIDA online database and represent the most recent values. The model predictions for cold core conditions and for when considering only gas-phase processes were computed as a function of time and compared to the predictions obtained with the previous version, kida.uva.2014. In addition, key chemical reactions were identified. The model predictions, including both gas and surface processes, were compared to the molecular abundances as observed in the cold core TMC1-CP. Many gas-phase reactions were revised or added to produce kida.uva.2024. The new model predictions are different by several orders of magnitude for some species. The agreement of this new model with observations in TMC-1 (CP) is, however, similar to the one obtained with the previous network.","PeriodicalId":8585,"journal":{"name":"Astronomy & Astrophysics","volume":"16 11","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-07-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141816925","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-07-22DOI: 10.1051/0004-6361/202451365
J. B'etrisey, Martin Farnir, S. Breton, Rafael A. Garc'ia, A. Broomhall, A. Amarsi, Oleg Kochukhov
Asteroseismic modelling will play a key role in future space-based missions, such as PLATO, CubeSpec, and Roman. Despite remarkable achievements, asteroseismology has revealed significant discrepancies between observations and theoretical predictions of the physics used in stellar models, which have the potential to bias stellar characterisation at the precision level demanded by PLATO. The current modelling strategies largely overlook magnetic activity, assuming that its effects are masked within the parametrisation of the so-called `surface effects'. Given the presence of activity cycles in multiple solar-like oscillators and activity variations in a significant fraction of Kepler observations of main-sequence stars, it is therefore relevant to investigate systematic errors in asteroseismic characterisations caused by our incomplete understanding of magnetic activity. Based on 26.5 years of GOLF and BiSON observations, we measured the impact of magnetic activity on the asteroseismic characterisation of the Sun as a star, a reference target for assessing the PLATO mission requirements. The GOLF and BiSON observations, which fully cover solar cycles 23 and 24, were divided into yearly overlapping snapshots, each delayed by a quarter of a year. For each snapshot, an advanced asteroseismic characterisation, similar to that to be adopted by the PLATO pipeline, was performed with standard prescriptions for the parametrisation of the surface effects. This allowed us to monitor the apparent temporal evolution of fundamental solar parameters such as mass, radius, and age. The correlation of these parameters with the 10.7 cm radio emission flux, a proxy of the solar activity cycle, was then measured. The effects of magnetic activity are partially absorbed into the parametrisation of the surface effects when suitable prescriptions are used, and they do not significantly affect the measured solar mass or radius. However, contrary to literature expectations, we find a significant imprint on the age determination, with variations of up to 6.5 between solar minima and maxima. This imprint persists across both BiSON and GOLF datasets. Considering that the Sun exhibits low levels of activity, our study highlights the looming challenge posed by magnetic activity for future photometry missions, and it prompts a potential reevaluation of the asteroseismic characterisation of the most active Kepler targets.
{"title":"Imprint of the magnetic activity cycle on solar asteroseismic characterisation based on 26 years of GOLF and BiSON data","authors":"J. B'etrisey, Martin Farnir, S. Breton, Rafael A. Garc'ia, A. Broomhall, A. Amarsi, Oleg Kochukhov","doi":"10.1051/0004-6361/202451365","DOIUrl":"https://doi.org/10.1051/0004-6361/202451365","url":null,"abstract":"Asteroseismic modelling will play a key role in future space-based missions, such as PLATO, CubeSpec, and Roman. Despite remarkable achievements, asteroseismology has revealed significant discrepancies between observations and theoretical predictions of the physics used in stellar models, which have the potential to bias stellar characterisation at the precision level demanded by PLATO. The current modelling strategies largely overlook magnetic activity, assuming that its effects are masked within the parametrisation of the so-called `surface effects'. Given the presence of activity cycles in multiple solar-like oscillators and activity variations in a significant fraction of Kepler observations of main-sequence stars, it is therefore relevant to investigate systematic errors in asteroseismic characterisations caused by our incomplete understanding of magnetic activity. Based on 26.5 years of GOLF and BiSON observations, we measured the impact of magnetic activity on the asteroseismic characterisation of the Sun as a star, a reference target for assessing the PLATO mission requirements. The GOLF and BiSON observations, which fully cover solar cycles 23 and 24, were divided into yearly overlapping snapshots, each delayed by a quarter of a year. For each snapshot, an advanced asteroseismic characterisation, similar to that to be adopted by the PLATO pipeline, was performed with standard prescriptions for the parametrisation of the surface effects. This allowed us to monitor the apparent temporal evolution of fundamental solar parameters such as mass, radius, and age. The correlation of these parameters with the 10.7 cm radio emission flux, a proxy of the solar activity cycle, was then measured. The effects of magnetic activity are partially absorbed into the parametrisation of the surface effects when suitable\u0000prescriptions are used, and they do not significantly affect the measured solar mass or radius. However, contrary to literature expectations, we find a significant imprint on the age determination, with variations of up to 6.5 between solar minima and maxima. This imprint persists across both BiSON and GOLF datasets. Considering that the Sun exhibits low levels of activity, our study highlights the looming challenge posed by magnetic activity for future photometry missions, and it prompts a potential reevaluation of the asteroseismic characterisation of the most active Kepler targets.","PeriodicalId":8585,"journal":{"name":"Astronomy & Astrophysics","volume":"22 1","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-07-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141815961","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-07-21DOI: 10.1051/0004-6361/202451256
J.Cernicharo, C.Cabezas, M. Ag'undez, R. Fuentetaja, B. Tercero, N. Marcelino, P. D. Vicente
We present the detection of the free radicals NC$_3$S and HC$_3$S towards TMC-1 with the QUIJOTE line survey. The derived column densities are (1.4pm 0.2)times 1011 for NC$_3$S and (1.5pm 0.2)times 1011 for HC$_3$S. We searched for NCCS, but only three transitions are within the domain of our QUIJOTE line survey and the observed lines are marginally detected at the 3sigma level, providing an upper limit to its column density of leq 6times 1010 cm$^ $. We also unsuccessfully searched for longer species of the NC$_n$S (nge 4) and HC$_n$S (nge 5) families in our TMC-1 data. A chemical model based on a reduced set of reactions involving HC$_3$S and NC$_3$S predicts abundances that are 10-100 times below the observed values. These calculations indicate that the most efficient reactions of formation of HC$_3$S and NC$_3$S in the model are S + C$_3$H$_2$ and N + HC$_3$S, respectively, while both radicals are very efficiently destroyed through reactions with neutral atoms.
{"title":"More sulphur in TMC-1: Discovery of the NC_3S and HC_3S radicals with the QUIJOTE line survey","authors":"J.Cernicharo, C.Cabezas, M. Ag'undez, R. Fuentetaja, B. Tercero, N. Marcelino, P. D. Vicente","doi":"10.1051/0004-6361/202451256","DOIUrl":"https://doi.org/10.1051/0004-6361/202451256","url":null,"abstract":"We present the detection of the free radicals NC$_3$S and HC$_3$S towards TMC-1\u0000with the QUIJOTE line survey. The derived column densities are (1.4pm 0.2)times 1011 for NC$_3$S and \u0000(1.5pm 0.2)times 1011 for HC$_3$S. We searched for NCCS, but only three transitions are within the \u0000domain of our QUIJOTE line\u0000survey and the observed lines are marginally detected at the 3sigma level, providing an upper limit to its \u0000column density of leq 6times 1010 cm$^ $.\u0000We also unsuccessfully searched for longer species of the NC$_n$S (nge 4) and HC$_n$S (nge 5)\u0000families in our TMC-1 data. A chemical model based on \u0000a reduced set of reactions involving HC$_3$S and NC$_3$S predicts abundances that are 10-100 times \u0000below the observed values. These calculations indicate that the most efficient reactions of formation \u0000of HC$_3$S and NC$_3$S in the model are S + C$_3$H$_2$ and N + HC$_3$S, respectively, while both radicals \u0000are very efficiently \u0000destroyed through reactions with neutral atoms.","PeriodicalId":8585,"journal":{"name":"Astronomy & Astrophysics","volume":"80 21","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-07-21","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141818849","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-07-20DOI: 10.1051/0004-6361/202449753
Valentina Sheminova, M. Baratella, V. D’Orazi
The primary objective of this study is to accurately determine the abundances of Cu, Sr, Y, Zr, Ba, La, and Ce in selected solar-type stars. This will allow us to establish observational abundance--metallicity and abundance--age relations and to explore the reasons for the excess of Ba compared to other $s$-elements in younger solar-type stars. The chosen $s$-process elements are critical diagnostics for understanding the chemical evolution of our Galaxy. We analysed HARPS spectra with a high resolution ($R$ = 115,000) and high signal-to-noise ratio (close to 100) of main-sequence solar-type FGK stars with metallicities from $-0.15$ to +0.35 dex and ages from 2 to 14 Gyr using one-dimensional (1D) local thermodynamic equilibrium (LTE) synthesis and MARCS atmospheric models. In the procedure of fitting synthetic to observed line profiles, the free parameters included abundance and microturbulent and macroturbulent velocity. The macroturbulent velocity can substantially compensate for non-local thermodynamic equilibrium (NLTE) effects in the line core. The resulting elemental abundance X/H increases with metallicity and age for solar-type stars. The ratio of the abundances of $s$-process elements s/Fe increases with decreasing metallicity and age, while the Cu/Fe ratio increases with both metallicity and age. These observed trends agree well with published observational data and with predictions from Galactic chemical evolution (GCE) models. A small Ba/Fe enhancement of 0.08 ± 0.08 dex has been detected in seven younger stars with an average age of $2.8 0.6$ Gyr. Compared to the abundances of other $s$-process elements Ba/Fe is 0.07 and 0.08 dex higher than La and Ce on average, respectively. Furthermore, we find that the Ba/Fe ratio increases with increasing chromospheric activity. The average Ba/Fe for the three most active stars is $0.15 0.10$ dex higher than that of the other stars. Chromospheric activity, characterised by stronger magnetic fields found in active regions such as pores, spots, plages, and networks, can significantly alter the physical conditions in the formation layers of the Ba lines. Our primary conclusion is that to account for the observed excess of Ba/Fe abundance in younger stars, it is essential to use more complex atmospheric models that incorporate magnetic structures.
{"title":"Abundances of neutron-capture elements in selected solar-type stars","authors":"Valentina Sheminova, M. Baratella, V. D’Orazi","doi":"10.1051/0004-6361/202449753","DOIUrl":"https://doi.org/10.1051/0004-6361/202449753","url":null,"abstract":"The primary objective of this study is to accurately determine the abundances of Cu, Sr, Y, Zr, Ba, La, and Ce in selected solar-type stars. This will allow us to establish observational abundance--metallicity and abundance--age relations and to explore the reasons for the excess of Ba compared to other $s$-elements in younger solar-type stars. The chosen $s$-process elements are critical diagnostics for understanding the chemical evolution of our Galaxy. We analysed HARPS spectra with a high resolution ($R$ = 115,000) and high signal-to-noise ratio (close to 100) of main-sequence solar-type FGK stars with metallicities from $-0.15$ to +0.35 dex and ages from 2 to 14 Gyr using one-dimensional (1D) local thermodynamic equilibrium (LTE) synthesis and MARCS atmospheric models. In the procedure of fitting synthetic to observed line profiles, the free parameters included abundance and microturbulent and macroturbulent velocity. The macroturbulent velocity can substantially compensate for non-local thermodynamic equilibrium (NLTE) effects in the line core. The resulting elemental abundance X/H increases with metallicity and age for solar-type stars.\u0000The ratio of the abundances of $s$-process elements s/Fe increases with decreasing metallicity and age, while the Cu/Fe ratio increases with both metallicity and age. These observed trends agree well with published observational data and with predictions from Galactic chemical evolution (GCE) models. A small Ba/Fe enhancement of 0.08 ± 0.08 dex has been detected in seven younger stars with an average age of $2.8 0.6$ Gyr. Compared to the abundances of other $s$-process elements Ba/Fe is 0.07 and 0.08 dex higher than La and Ce on average, respectively. Furthermore, we find that the Ba/Fe ratio increases with increasing chromospheric activity.\u0000The average Ba/Fe for the three most active stars is $0.15 0.10$ dex higher than that of the other stars. Chromospheric activity, characterised by stronger magnetic fields found in active regions such as pores, spots, plages, and networks, can significantly alter the physical conditions in the formation layers of the Ba lines. Our primary conclusion is that to account for the observed excess of Ba/Fe abundance in younger stars, it is essential to use more complex atmospheric models that incorporate magnetic structures.","PeriodicalId":8585,"journal":{"name":"Astronomy & Astrophysics","volume":"23 2","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-07-20","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141819511","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-07-20DOI: 10.1051/0004-6361/202450638
C. Guerra, Z. Meliani, G. Voisin
The detected population of "spiders", referring to millisecond pulsar binaries, has significantly grown in the past decade thanks to multiwavelength follow-up investigations of unidentified Fermi sources. These systems consist of low-mass stellar companions orbiting rotation-powered millisecond pulsars in short periods of a few hours up to day. Among them, a subset of intriguing objects called transitional millisecond pulsars (tMSPs) has been shown to exhibit a remarkable behavior, transitioning between pulsar-binary and faint low-mass X-ray binary states over a span of a few years. Our objective is to study the interaction of stellar winds in tMSPs in order to understand their observational properties. To this end we focus on the parameter range that places the system near Roche-lobe overflow. Employing the adaptative mesh refinement (AMR) AMRVAC 2.0 code, we performed 2D hydrodynamical (HD) simulations of the interaction between the flows from both stars, accounting for the effects of gravity and orbital motion. By studying the mass loss and launch speed of the winds, we successfully recreated two phenomenologically distinct regimes: the accretion stream and the pulsar radio state. We also identified the tipping point that marks the sharp transition between these two states. In the accretion stream state, we discover a very strong variability induced by the pulsar wind. In the pulsar state, we reconstructed the corresponding X-ray light curves of the system that produces the characteristic double-peak pattern of these systems. The position of the peaks is shifted due to orbital motion and the leading peak is weaker due to eclipsing by the companion. This study highlights the importance of gravity and orbital motion in the interaction between the companion and pulsar winds. Our setup allows the study of the complex interaction between the pulsar wind and an accretion stream during mass transfer. We suggest that a smaller leading peak in X-rays is indicative of a nearly edge-on system.
在过去十年中,由于对费米不明来源进行了多波长跟踪调查,所探测到的 "蜘蛛"(指毫秒脉冲星双星)数量有了显著增加。这些系统由低质量恒星伴星组成,在几小时到一天的短周期内围绕旋转动力毫秒脉冲星运行。在这些天体中,有一个名为 "过渡毫秒脉冲星"(transitional millisecond pulsars,tMSPs)的有趣天体子集表现出了非凡的行为,它们在脉冲星-双星状态和微弱的低质量 X 射线双星状态之间的转换时间跨度长达数年。我们的目标是研究 tMSPs 中恒星风的相互作用,以了解它们的观测特性。为此,我们重点研究了将系统置于罗氏环溢出附近的参数范围。利用自适应网格细化(AMR)AMRVAC 2.0 代码,我们对来自两颗恒星的气流之间的相互作用进行了二维流体力学(HD)模拟,并考虑了重力和轨道运动的影响。通过研究质量损失和风的发射速度,我们成功地再现了两种现象截然不同的状态:吸积流和脉冲星射电状态。我们还确定了标志着这两种状态急剧转变的临界点。在吸积流状态下,我们发现了由脉冲星风引起的非常强的变异性。在脉冲星状态下,我们重建了系统的相应 X 射线光曲线,它产生了这些系统特有的双峰模式。由于轨道运动,峰值的位置发生了偏移,并且由于伴星的食蚀作用,前导峰值变弱了。这项研究强调了引力和轨道运动在伴星与脉冲星风相互作用中的重要性。我们的装置可以研究质量转移过程中脉冲星风和吸积流之间复杂的相互作用。我们认为,X 射线中较小的前沿峰值表明这是一个接近边缘的系统。
{"title":"Hydrodynamical simulations of wind interaction in spider systems. A step toward understanding transitional millisecond pulsars","authors":"C. Guerra, Z. Meliani, G. Voisin","doi":"10.1051/0004-6361/202450638","DOIUrl":"https://doi.org/10.1051/0004-6361/202450638","url":null,"abstract":"The detected population of \"spiders\", referring to millisecond pulsar binaries, has significantly grown in the past decade thanks to multiwavelength follow-up investigations of unidentified Fermi sources. These systems consist of low-mass stellar companions orbiting rotation-powered millisecond pulsars in short periods of a few hours up to day. Among them, a subset of intriguing objects called transitional millisecond pulsars (tMSPs) has been shown to exhibit a remarkable behavior, transitioning between pulsar-binary and faint low-mass X-ray binary states over a span of a few years. Our objective is to study the interaction of stellar winds in tMSPs in order to understand their observational properties. To this end we focus on the parameter range that places the system near Roche-lobe overflow. Employing the adaptative mesh refinement (AMR) AMRVAC 2.0 code, we performed 2D hydrodynamical (HD) simulations of the interaction between the flows from both stars, accounting for the effects of gravity and orbital motion. By studying the mass loss and launch speed of the winds, we successfully recreated two phenomenologically distinct regimes: the accretion stream and the pulsar radio state. We also identified the tipping point that marks the sharp transition between these two states. In the accretion stream state, we discover a very strong variability induced by the pulsar wind. In the pulsar state, we reconstructed the corresponding X-ray light curves of the system that produces the characteristic double-peak pattern of these systems. The position of the peaks is shifted due to orbital motion and the leading peak is weaker due to eclipsing by the companion. This study highlights the importance of gravity and orbital motion in the interaction between the companion and pulsar winds.\u0000 Our setup allows the study of the complex interaction between the pulsar wind and an accretion stream during mass transfer.\u0000 We suggest that a smaller leading peak in X-rays is indicative of a nearly edge-on system.","PeriodicalId":8585,"journal":{"name":"Astronomy & Astrophysics","volume":"125 10","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-07-20","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141819549","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-07-19DOI: 10.1051/0004-6361/202450078
J. Kanwar, I. Kamp, H. Jang, L. Waters, E. V. Dishoeck, V. Christiaens, A. M. Arabhavi, Thomas K. Henning, M. Gudel, P. Woitke, Olivier Absil, D. Barrado, A. C. O. Garatti, A. Glauser, F. Lahuis, S. Scheithauer, B. Vandenbussche, D. Gasman, S. Grant, N. Kurtovic, G. Perotti, B. Tabone, M. Temmink
With the advent of JWST, we are acquiring unprecedented insights into the physical and chemical structure of the inner regions of planet-forming disks where terrestrial planet formation occurs. Very low-mass stars (VLMSs) are known to have a high occurrence of the terrestrial planets orbiting them. Exploring the chemical composition of the gas in these inner disk regions can help us better understand the connection between planet-forming disks and planets. sun We used the dust-fitting tool DuCK to determine the dust continuum and to place constraints on the dust composition and grain sizes. We used 0D slab models to identify and fit the molecular spectral features, which yielded estimates on the temperature, column density, and emitting area. To test our understanding of the chemistry in the disks around VLMSs, we employed the thermo-chemical disk model P RO D I M O and investigated the reservoirs of the detected hydrocarbons. We explored how the C/O ratio affects the inner disk chemistry. JWST reveals a plethora of hydrocarbons, including CH3 CH4 C2H2 CCH2 C2H6 C3H4 C4H2 and C6H6 which suggests a disk with a gaseous C/O,>,1. Additionally, we detect CO2 CO2 HCN and HC3N H2O and OH are absent from the spectrum. We do not detect polycyclic aromatic hydrocarbons. Photospheric stellar absorption lines of H2O and CO are identified. Notably, our radiation thermo-chemical disk models are able to produce these detected hydrocarbons in the surface layers of the disk when C/O,>,1. The presence of C C+ H, and H2 is crucial for the formation of hydrocarbons in the surface layers, and a C/O ratio larger than 1 ensures the surplus of C needed to drive this chemistry. Based on this, we predict a list of additional hydrocarbons that should also be detectable. Both amorphous and crystalline silicates (enstatite and forsterite) are present in the disk and we find grain sizes of 2 and 5,mu m. The disk around Sz28 is rich in hydrocarbons, and its inner regions have a high gaseous C/O ratio. In contrast, it is the first VLMS disk in the MINDS sample to show both distinctive dust features and a rich hydrocarbon chemistry. The presence of large grains indicates dust growth and evolution. Thermo-chemical disk models that employ an extended hydrocarbon chemical network together with C/O,>1 are able to explain the hydrocarbon species detected in the spectrum.
随着 JWST 的问世,我们对行星形成盘内部区域的物理和化学结构有了前所未有的深入了解。众所周知,超低质量恒星(VLMSs)中有大量的类地行星围绕它们运行。探索这些内盘区域气体的化学成分有助于我们更好地理解行星形成盘与行星之间的联系。 我们使用尘埃拟合工具 DuCK 来确定尘埃连续面,并对尘埃成分和粒度进行约束。我们使用 0D 板坯模型来识别和拟合分子光谱特征,从而对温度、柱密度和发射区域做出估计。为了检验我们对 VLMSs 周围磁盘化学性质的理解,我们使用了热化学磁盘模型 P RO D I M O,并对探测到的碳氢化合物的储层进行了研究。我们探讨了C/O比如何影响内盘化学。JWST发现了大量碳氢化合物,包括CH3 CH4 C2H2 CCH2 C2H6 C3H4 C4H2和C6H6。此外,我们还探测到 CO2 CO2 HCN 和 HC3N H2O,光谱中没有 OH。我们没有探测到多环芳烃。光层恒星吸收线 H2O 和 CO 被识别出来。值得注意的是,当C/O,>,1时,我们的辐射热化学盘模型能够在盘的表层产生这些探测到的碳氢化合物。C C+ H和H2的存在对于表层碳氢化合物的形成至关重要,而大于1的C/O比确保了驱动这种化学反应所需的过剩C。在此基础上,我们预测了一系列也应该可以检测到的其他碳氢化合物。Sz28周围的圆盘富含碳氢化合物,其内部区域具有较高的气态C/O比。相比之下,它是MINDS样本中第一个同时显示出独特的尘埃特征和丰富的碳氢化合物化学成分的VLMS盘。大颗粒的存在表明了尘埃的生长和演化。采用扩展碳氢化合物化学网络和 C/O(>1)的热化学盘模型能够解释光谱中探测到的碳氢化合物种类。
{"title":"MINDS. Hydrocarbons detected by JWST/MIRI in the inner disk of Sz28 consistent with a high C/O gas-phase chemistry","authors":"J. Kanwar, I. Kamp, H. Jang, L. Waters, E. V. Dishoeck, V. Christiaens, A. M. Arabhavi, Thomas K. Henning, M. Gudel, P. Woitke, Olivier Absil, D. Barrado, A. C. O. Garatti, A. Glauser, F. Lahuis, S. Scheithauer, B. Vandenbussche, D. Gasman, S. Grant, N. Kurtovic, G. Perotti, B. Tabone, M. Temmink","doi":"10.1051/0004-6361/202450078","DOIUrl":"https://doi.org/10.1051/0004-6361/202450078","url":null,"abstract":"With the advent of JWST, we are acquiring unprecedented insights into the physical and chemical structure of the inner regions of planet-forming disks where terrestrial planet formation occurs. Very low-mass stars (VLMSs) are known to have a high occurrence of the terrestrial planets orbiting them. Exploring the chemical composition of the gas in these inner disk regions can help us better understand the connection between planet-forming disks and planets. sun We used the dust-fitting tool DuCK to determine the dust continuum and to place constraints on the dust composition and grain sizes. We used 0D slab models to identify and fit the molecular spectral features, which yielded estimates on the temperature, column density, and emitting area. To test our understanding of the chemistry in the disks around VLMSs, we employed the thermo-chemical disk model P RO D I M O and investigated the reservoirs of the detected hydrocarbons. We explored how the C/O ratio affects the inner disk chemistry. JWST reveals a plethora of hydrocarbons, including CH3 CH4 C2H2 CCH2 C2H6 C3H4 C4H2 and C6H6 which suggests a disk with a gaseous C/O,>,1. Additionally, we detect CO2 CO2 HCN and HC3N H2O and OH are absent from the spectrum. We do not detect polycyclic aromatic hydrocarbons. Photospheric stellar absorption lines of H2O and CO are identified. Notably, our radiation thermo-chemical disk models are able to produce these detected hydrocarbons in the surface layers of the disk when C/O,>,1. The presence of C C+ H, and H2 is crucial for the formation of hydrocarbons in the surface layers, and a C/O ratio larger than 1 ensures the surplus of C needed to drive this chemistry. Based on this, we predict a list of additional hydrocarbons that should also be detectable. Both amorphous and crystalline silicates (enstatite and forsterite) are present in the disk and we find grain sizes of 2 and 5,mu m. The disk around Sz28 is rich in hydrocarbons, and its inner regions have a high gaseous C/O ratio. In contrast, it is the first VLMS disk in the MINDS sample to show both distinctive dust features and a rich hydrocarbon chemistry. The presence of large grains indicates dust growth and evolution. Thermo-chemical disk models that employ an extended hydrocarbon chemical network together with C/O,>1 are able to explain the hydrocarbon species detected in the spectrum.","PeriodicalId":8585,"journal":{"name":"Astronomy & Astrophysics","volume":"108 46","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-07-19","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141821508","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-07-19DOI: 10.1051/0004-6361/202450902
V. S. Veena, W.-J. Kim, Á. Sánchez-Monge, P. Schilke, K. Menten, G. Fuller, M. Sormani, F. Wyrowski, W. E. Banda-Barragan, D. Riquelme, P. Tarrio, P. D. Vicente
The expanding molecular ring (EMR) manifests itself as a parallelogram in the position-velocity diagram of spectral line emission from the Central Molecular Zone (CMZ) surrounding the Galactic centre (GC). It is a high velocity ($ V_ LSR extended molecular gas structure. The formation of the EMR is believed to be associated with the bar driven inflow onto the nuclear region of the Galaxy. The physical and chemical properties, as well as the evolution of the EMR and its connection to other GC clouds and the CMZ as a whole, are not yet fully comprehended. Using multiwavelength data, we investigate the gas kinematics, star formation activity, and the presence of shocked gas in a 200 pc long high velocity gas stream (V$_ LSR with a double helix morphology named the helix stream, that is located 15--55 pc above the CMZ ($l $b and is kinematically associated with the EMR/parallelogram. To study the kinematics of the helix stream, we used 13CO ($J=2-1$) data from the SEDIGISM survey and 12CO ($J=1-0$) archival data from the Nobeyama telescope. Additional multiwavelength archival data from infrared to radio wavelengths were used to investigate the star formation activity. We carried out molecular line observations using the IRAM 30m, Yebes 40m, and APEX 12m telescopes. The detection of four rotational transitions of the SiO molecule ($J=$ 1--0, 2--1, 5--4, 7--6) indicate the presence of shocks. We derived the SiO column densities and abundances in different regions of the helix stream using the rotational diagram method. We also performed non-local thermodynamic equilibrium (non-LTE) modelling of the SiO emission to analyse the excitation conditions of the shocked gas. The presence of clumps with submillimetre continuum emission from dust and a candidate region signify the ongoing star formation activity within the helix stream. The cloud is massive ($2.5 M$_ and highly turbulent ($ V mean We find evidence of cloud-cloud collisions towards the eastern edge ($l suggesting a dynamic interaction with the CMZ. An expanding shell is detected within the cloud with radius of 6.7 pc and an expansion velocity of 35 The shell might be powered by several supernovae or a single hypernova. The relative abundance of SiO within the helix stream with respect to H$_2$ implies extensive shock processes occurring on large scales ($X$(SiO) $ $). The helical or cork-screw velocity structure observed within the individual strands of the helix stream indicates twisting and turning motions occurring within the cloud. We propose that the helix stream is the continuation of the near side bar lane, that is overshooting after ``brushing'' the CMZ and interacting with it at the location of the G1.3 cloud. This interpretation finds support both from numerical simulations and prior observational studies of the CMZ. Our findings carry profound implications for understanding star formation in extreme conditions and they elucidate the intricate properties of gas and dust associated wit
{"title":"Star formation in extreme environments: A 200 pc high velocity gas stream in the Galactic centre","authors":"V. S. Veena, W.-J. Kim, Á. Sánchez-Monge, P. Schilke, K. Menten, G. Fuller, M. Sormani, F. Wyrowski, W. E. Banda-Barragan, D. Riquelme, P. Tarrio, P. D. Vicente","doi":"10.1051/0004-6361/202450902","DOIUrl":"https://doi.org/10.1051/0004-6361/202450902","url":null,"abstract":"The expanding molecular ring (EMR) manifests itself as a parallelogram in the position-velocity diagram of spectral line emission from the Central Molecular Zone (CMZ) surrounding the Galactic centre (GC). It is a high velocity ($ V_ LSR extended molecular gas structure. The formation of the EMR is believed to be associated with the bar driven inflow onto the nuclear region of the Galaxy. The physical and chemical properties, as well as the evolution of the EMR and its connection to other GC clouds and the CMZ as a whole, are not yet fully comprehended. Using multiwavelength data, we investigate the gas kinematics, star formation activity, and the presence of shocked gas in a 200 pc long high velocity gas stream (V$_ LSR with a double helix morphology named the helix stream, that is located 15--55 pc above the CMZ ($l $b and is kinematically associated with the EMR/parallelogram. To study the kinematics of the helix stream, we used 13CO ($J=2-1$) data from the SEDIGISM survey and 12CO ($J=1-0$) archival data from the Nobeyama telescope. Additional multiwavelength archival data from infrared to radio wavelengths were used to investigate the star formation activity. We carried out molecular line observations using the IRAM 30m, Yebes 40m, and APEX 12m telescopes. The detection of four rotational transitions of the SiO molecule ($J=$ 1--0, 2--1, 5--4, 7--6) indicate the presence of shocks. We derived the SiO column densities and abundances in different regions of the helix stream using the rotational diagram method. We also performed non-local thermodynamic equilibrium (non-LTE) modelling of the SiO emission to analyse the excitation conditions of the shocked gas. The presence of clumps with submillimetre continuum emission from dust and \u0000 a candidate region signify the ongoing star formation activity within the helix stream. The cloud is massive ($2.5 M$_ and highly turbulent ($ V mean We find evidence of cloud-cloud collisions towards the eastern edge ($l suggesting a dynamic interaction with the CMZ. An expanding shell is detected within the cloud with radius of 6.7 pc and an expansion velocity of 35 The shell might be powered by several supernovae or a single hypernova. The relative abundance of SiO within the helix stream with respect to H$_2$ implies extensive shock processes occurring on large scales ($X$(SiO) $ $). The helical or cork-screw velocity structure observed within the individual strands of the helix stream indicates twisting and turning motions occurring within the cloud. We propose that the helix stream is the continuation of the near side bar lane, that is overshooting after ``brushing'' the CMZ and interacting with it at the location of the G1.3 cloud. This interpretation finds support both from numerical simulations and prior observational studies of the CMZ. Our findings carry profound implications for understanding star formation in extreme conditions and they elucidate the intricate properties of gas and dust associated wit","PeriodicalId":8585,"journal":{"name":"Astronomy & Astrophysics","volume":"122 11","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-07-19","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141821951","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}