Pub Date : 2024-07-29DOI: 10.1051/0004-6361/202449659
J. Greiner, T. Kruhler, J. Bolmer, S. Klose, P. Afonso, J. Elliott, R. Filgas, J. Graham, D. A. Kann, F. Knust
A dedicated gamma-ray burst (GRB) afterglow observing program was performed between 2007 and 2016 with GROND, a seven-channel optical and near-infrared imager at the 2.2m telescope of the Max-Planck Society at ESO/La Silla, In this first of a series of papers, we describe the GRB observing plan, providing first readings of all so far unpublished GRB afterglow measurements and some observing statistics. In total, we observed 514 GRBs with GROND, including 434 Swift -detected GRBs, representing 81 of the observable Swift sample. For GROND-observations within 30 min of the GRB trigger, the optical/NIR afterglow detection rate is 81 for long- and 57 for short-duration GRBs. We report the discovery of ten new GRB afterglows plus one candidate, along with redshift estimates (partly improved) for four GRBs and new host detections for seven GRBs. We identify the (already known) afterglow of GRB 140209A as the sixth GRB exhibiting a 2175 dust feature. As a side result, we identified two blazars, with one at a redshift of z=3.8 (in the GRB 131209A field).
在本系列论文的第一篇中,我们介绍了伽玛射线暴(GRB)观测计划,提供了迄今为止尚未发表的所有伽玛射线暴余辉测量数据的首次读数以及一些观测统计数据。我们总共利用 GROND 观测了 514 个 GRB,其中包括 434 个 Swift 检测到的 GRB,占 Swift 可观测样本的 81%。对于在GRB触发后30分钟内进行的GROND观测,光学/近红外余辉的探测率为:长持续时间GRB 81个,短持续时间GRB 57个。我们报告发现了 10 个新的 GRB 余辉和一个候选余辉,同时还对 4 个 GRB 进行了红移估算(部分改进),并对 7 个 GRB 进行了新的宿主探测。我们发现(已经知道的)GRB 140209A 的余辉是第六个表现出 2175 尘埃特征的 GRB。另外,我们还发现了两颗类星体,其中一颗的红移为 z=3.8(在 GRB 131209A 星场内)。
{"title":"The GROND gamma-ray burst sample I. Overview and statistics","authors":"J. Greiner, T. Kruhler, J. Bolmer, S. Klose, P. Afonso, J. Elliott, R. Filgas, J. Graham, D. A. Kann, F. Knust","doi":"10.1051/0004-6361/202449659","DOIUrl":"https://doi.org/10.1051/0004-6361/202449659","url":null,"abstract":"A dedicated\u0000 gamma-ray burst (GRB) afterglow observing program was performed between 2007 and 2016 with GROND, a seven-channel optical and near-infrared imager at the \u0000 2.2m telescope of the Max-Planck Society at ESO/La Silla, \u0000 In this first of a series of papers, we describe the GRB observing plan,\u0000 providing first readings of all so far unpublished GRB afterglow measurements\u0000 and some observing statistics.\u0000 In total, we observed 514 GRBs with GROND, including 434 Swift -detected GRBs, representing 81 of the observable Swift sample.\u0000 For GROND-observations within 30 min of the GRB trigger, the optical/NIR\u0000 afterglow detection rate is 81 for long- and 57 for short-duration GRBs.\u0000 We report the discovery of ten new GRB\u0000 afterglows plus one candidate, along with redshift estimates (partly improved)\u0000 for four GRBs and new host detections for seven GRBs.\u0000 We identify the (already known) afterglow of GRB 140209A\u0000 as the sixth GRB exhibiting a 2175 dust feature. As a side result, we identified two blazars, with one at a redshift of z=3.8 (in the GRB 131209A field).","PeriodicalId":8585,"journal":{"name":"Astronomy & Astrophysics","volume":"28 2","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-07-29","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141796755","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 : 2024-07-26DOI: 10.1051/0004-6361/202450047
M. Mallorquín, V. J. S. Béjar, N. Lodieu, M. Z. Zapatero Osorio, H. Yu, A. Suárez Mascareño, M. Damasso, J. Sanz-Forcada, I. Ribas, A. Reiners, A. Quirrenbach, P. Amado, J. A. Caballero, S. Aigrain, O. Barragán, S. Dreizler, Á. Fernández-Martín, E. Goffo, T. Henning, A. Kaminski, B. Klein, R. Luque, D. Montes, J. C. Morales, E. Nagel, E. Pallé, S. Reffert, M. Schlecker, A. Schweitzer
Understanding planet formation is important in the context of the origin of planetary systems in general and of the Solar System in particular, as well as to predict the likelihood of finding Jupiter, Neptune, and Earth analogues around other stars. We aim to precisely determine the radii and dynamical masses of transiting planets orbiting the young M star AU,Mic using public photometric and spectroscopic datasets. We performed a joint fit analysis of the TESS and CHEOPS light curves and more than 400 high-resolution spectra collected with several telescopes and instruments. We characterise the stellar activity and physical properties (radius, mass, density) of the transiting planets in the young AU,Mic system through joint transit and radial velocity fits with Gaussian processes. We determine a radius of $R_ p b $=,4.79,pm ,0.29 R$_ a mass of p b $=,9.0,pm ,2.7 M$_ and a bulk density of $ p b $,=,0.49,pm ,0.16 $ for the innermost transiting planet AU,Mic,b. For the second known transiting planet, AU,Mic,c, we infer a radius of p c $=,2.79,pm ,0.18 R$_ a mass of p c $=,14.5,pm ,3.4 M$_ and a bulk density of $ p c $,=,3.90,pm ,1.17 $. According to theoretical models, AU,Mic,b may harbour an $ envelope larger than 5 by mass, with a fraction of rock and a fraction of water. AU,Mic,c could be made of rock and/or water and may have an $ atmosphere comprising at most 5 of its mass. AU,Mic,b has retained most of its atmosphere but might lose it over tens of millions of years due to the strong stellar radiation, while AU,Mic,c likely suffers much less photo-evaporation because it lies at a larger separation from its host. Using all the datasets in hand, we determine a 3sigma upper mass limit of p d i oplus $ for the AU,Mic 'd' TTV-candidate. In addition, we do not confirm the recently proposed existence of the planet candidate AU,Mic,'e' with an orbital period of 33.4 days. We investigated the level of the radial velocity variations and show that it is lower at longer wavelength with smaller changes from one observational campaign to another.
了解行星的形成对于行星系统的起源,特别是太阳系的起源,以及预测在其他恒星周围发现木星、海王星和地球类似物的可能性都非常重要。我们的目标是利用公开的测光和光谱数据集精确测定围绕年轻 M 星 AU,Mic 的凌日行星的半径和动力质量。我们对TESS和CHEOPS的光变曲线以及由多个望远镜和仪器收集的400多条高分辨率光谱进行了联合拟合分析。我们用高斯过程联合拟合了年轻的AU/,Mic系统中凌日行星的恒星活动和物理性质(半径、质量、密度)。我们确定最内侧的凌星AU Mic b的半径为$R_ p b $=,4.79,pm ,0.29 R$_,质量为p b $=,9.0,pm ,2.7 M$_,体积密度为p b $=,0.49,pm ,0.16 $。对于第二颗已知的凌星AU,Mic,c,我们推断它的半径为p c $,2.79,pm ,0.18 R$_,质量为p c $,14.5,pm ,3.4 M$_,体积密度为p c $,=,3.90,pm ,1.17 $。根据理论模型,AU,Mic,b可能蕴藏着一个质量大于5的包络体,其中一部分是岩石,一部分是水。AU,Mic,c可能由岩石和/或水组成,可能有一个最多占其质量5的大气层。AU,Mic,b保留了大部分大气,但由于强烈的恒星辐射,它可能会在数千万年的时间里失去大气,而AU,Mic,c可能遭受的光蒸发要少得多,因为它与其宿主的距离较大。利用手头的所有数据集,我们为AU Mic 'd'TTV候选星确定了一个3西格玛质量上限,即p d i oplus $。此外,我们并没有证实最近提出的轨道周期为33.4天的候选行星AU,Mic,'e'的存在。我们对径向速度的变化水平进行了研究,结果表明,在较长的波长上,径向速度的变化水平较低,在不同的观测活动中,径向速度的变化较小。
{"title":"Revisiting the dynamical masses of the transiting planets in the young AU Mic system: Potential AU,Mic b inflation at sim 20 Myr","authors":"M. Mallorquín, V. J. S. Béjar, N. Lodieu, M. Z. Zapatero Osorio, H. Yu, A. Suárez Mascareño, M. Damasso, J. Sanz-Forcada, I. Ribas, A. Reiners, A. Quirrenbach, P. Amado, J. A. Caballero, S. Aigrain, O. Barragán, S. Dreizler, Á. Fernández-Martín, E. Goffo, T. Henning, A. Kaminski, B. Klein, R. Luque, D. Montes, J. C. Morales, E. Nagel, E. Pallé, S. Reffert, M. Schlecker, A. Schweitzer","doi":"10.1051/0004-6361/202450047","DOIUrl":"https://doi.org/10.1051/0004-6361/202450047","url":null,"abstract":"Understanding planet formation is important in the context of the origin of planetary systems in general and of the Solar System in particular, as well as to predict the likelihood of finding Jupiter, Neptune, and Earth analogues around other stars. We aim to precisely determine the radii and dynamical masses of transiting planets orbiting the young M star AU,Mic using public photometric and spectroscopic datasets. We performed a joint fit analysis of the TESS and CHEOPS light curves and more than 400 high-resolution spectra collected with several telescopes and instruments. We characterise the stellar activity and physical properties (radius, mass, density) of the transiting planets in the young AU,Mic system through joint transit and radial velocity fits with Gaussian processes. We determine a radius of $R_ p b $=,4.79,pm ,0.29 R$_ a mass of p b $=,9.0,pm ,2.7 M$_ and a bulk density of $ p b $,=,0.49,pm ,0.16 $ for the innermost transiting planet AU,Mic,b. For the second known transiting planet, AU,Mic,c, we infer a radius of p c $=,2.79,pm ,0.18 R$_ a mass of p c $=,14.5,pm ,3.4 M$_ and a bulk density of $ p c $,=,3.90,pm ,1.17 $. According to theoretical models, AU,Mic,b may harbour an $ envelope larger than 5 by mass, with a fraction of rock and a fraction of water. AU,Mic,c could be made of rock and/or water and may have an $ atmosphere comprising at most 5 of its mass. AU,Mic,b has retained most of its atmosphere but might lose it over tens of millions of years due to the strong stellar radiation, while AU,Mic,c likely suffers much less photo-evaporation because it lies at a larger separation from its host. Using all the datasets in hand, we determine a 3sigma upper mass limit of p d i oplus $ for the AU,Mic 'd' TTV-candidate. In addition, we do not confirm the recently proposed existence of the planet candidate AU,Mic,'e' with an orbital period of 33.4 days. We investigated the level of the radial velocity variations and show that it is lower at longer wavelength with smaller changes from one observational campaign to another.","PeriodicalId":8585,"journal":{"name":"Astronomy & Astrophysics","volume":"27 9","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-07-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141799251","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 : 2024-07-26DOI: 10.1051/0004-6361/202450815
M. A. Raj, P. Awad, R. Peletier, R. Smith, U. Kuchner, R. van de Weygaert, N.I. Libeskind, M. Canducci, P. Tino, K. Bunte
Our objectives are to map the filamentary network around the Fornax-Eridanus complex and probe the influence of the local environment on galaxy morphology. We employed the novel machine-learning tool, named, 1-Dimensional, Recovery, Extraction, and Analysis of Manifolds (1-DREAM) to detect and model filaments around the Fornax cluster. We then used the morphology-density relation of galaxies to examine the variation in the galaxies' morphology with respect to their distance from the central axis of the detected filaments. We detected 27 filaments that vary in length and galaxy-number density around the Fornax-Eridanus complex. We find that 81 of galaxies in our catalogue belong to filaments and 19 of galaxies are located outside filaments. The filaments around the Fornax-Eridanus complex showcase a variety of environments: some filaments encompass groups and clusters, while others are only inhabited by galaxies in pristine filamentary environments. In this context, we reveal a well-known structure, namely: the Fornax Wall, which passes through the Dorado group, Fornax cluster, and Eridanus supergroup. With regard to the morphology of galaxies, we find that early-type galaxies (ETGs) populate high-density filaments and high-density regions of the Fornax Wall. Furthermore, the fraction of the ETG-population decreases as the distance to the central axis of the filament increases. The fraction of late-type galaxies (LTGs; 8) is lower than that of ETGs (12) at 0.5 Mpc/$h$ from the filament spine. Of the total galaxy population in filaments around the Fornax-Eridanus complex, sim 7 are ETGs and sim 24 are LTGs located in pristine environments of filaments, while sim 27 are ETGs and sim 42 are LTGs in groups and clusters within filaments. Among the galaxies in the filamentary network around the Fornax-Eridanus complex, 44 of them belong to the Fornax Wall. This study reveals the cosmic web around the Fornax cluster, which exhibits a variety of filamentary environments. With this, our research asserts that filamentary environments are heterogeneous in nature. When investigating the role of the environment on galaxy morphology, it is essential to consider both the local number-density and a galaxy's proximity to the filament spine (i.e. the filament core). Within this framework, we ascribe the observed morphological segregation in the Fornax Wall to the pre-processing of galaxies among groups embedded in it.
{"title":"Large-scale structure around the Fornax-Eridanus complex","authors":"M. A. Raj, P. Awad, R. Peletier, R. Smith, U. Kuchner, R. van de Weygaert, N.I. Libeskind, M. Canducci, P. Tino, K. Bunte","doi":"10.1051/0004-6361/202450815","DOIUrl":"https://doi.org/10.1051/0004-6361/202450815","url":null,"abstract":"Our objectives are to map the filamentary network around the Fornax-Eridanus complex and probe the influence of the local environment on galaxy morphology. We employed the novel machine-learning tool, named, 1-Dimensional, Recovery, Extraction, and Analysis of Manifolds (1-DREAM) to detect and model filaments around the Fornax cluster. We then used the morphology-density relation of galaxies to examine the variation in the galaxies' morphology with respect to their distance from the central axis of the detected filaments. We detected 27 filaments that vary in length and galaxy-number density around the Fornax-Eridanus complex. We find that 81 of galaxies in our catalogue belong to filaments and 19 of galaxies are located outside filaments. The filaments around the Fornax-Eridanus complex showcase a variety of environments: some filaments encompass groups and clusters, while others are only inhabited by galaxies in pristine filamentary environments. In this context, we reveal a well-known structure, namely: the Fornax Wall, which passes through the Dorado group, Fornax cluster, and Eridanus supergroup. With regard to the morphology of galaxies, we find that early-type galaxies (ETGs) populate high-density filaments and high-density regions of the Fornax Wall. Furthermore, the fraction of the ETG-population decreases as the distance to the central axis of the filament increases. The fraction of late-type galaxies (LTGs; 8) is lower than that of ETGs (12) at 0.5 Mpc/$h$ from the filament spine. Of the total galaxy population in filaments around the Fornax-Eridanus complex, sim 7 are ETGs and sim 24 are LTGs located in pristine environments of filaments, while sim 27 are ETGs and sim 42 are LTGs in groups and clusters within filaments. Among the galaxies in the filamentary network around the Fornax-Eridanus complex, 44 of them belong to the Fornax Wall. This study reveals the cosmic web around the Fornax cluster, which exhibits a variety of filamentary environments. With this, our research asserts that filamentary environments are heterogeneous in nature. When investigating the role of the environment on galaxy morphology, it is essential to consider both the local number-density and a galaxy's proximity to the filament spine (i.e. the filament core). Within this framework, we ascribe the observed morphological segregation in the Fornax Wall to the pre-processing of galaxies among groups embedded in it.","PeriodicalId":8585,"journal":{"name":"Astronomy & Astrophysics","volume":"39 22","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-07-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141800221","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 : 2024-07-26DOI: 10.1051/0004-6361/202347583
N. Kurtovic, S. Facchini, M. Benisty, P. Pinilla, S. Cabrit, E.L.N. Jensen, C. Dougados, R. Booth, C. N. Kimmig, C. Manara, J. E. Rodriguez
The dynamical interactions between young binaries can perturb the material distribution of their circumstellar disks, and modify the planet formation process. In order to understand how planets form in multiple stellar systems, it is necessary to characterize both their binary orbit and their disks properties. In order to constrain the impact and nature of the binary interaction in the RW,Aur system (bound or unbound), we analyzed the circumstellar material at 1.3,mm wavelengths, as observed at multiple epochs by the Atacama Large (sub-)millimeter Array (ALMA). We analyzed the disk properties through parametric visibility modeling, and we used this information to constrain the dust morphology and the binary orbital period. We imaged the dust continuum emission of RW,Aur with a resolution of 3,au, and we find that the radius enclosing 90 of the flux 90 $) is 19,au and 14,au for RW,Aur,A and B, respectively. By modeling the relative distance of the disks at each epoch, we find a consistent trend of movement for the disk of RW,Aur,B moving away from the disk of RW,Aur,A at an approximate rate of $ in sky-projected distance). By combining ALMA astrometry, historical astrometry, and the dynamical masses of each star, we constrain the RW,Aur binary stars to be most likely in a high-eccentricity elliptical orbit with a clockwise prograde orientation relative to RW,Aur,A, although low-eccentricity hyperbolic orbits are not ruled out by the astrometry. Our analysis does not exclude the possibility of a disk collision during the last interaction, which occurred $,yr ago relative to beginning of 2024. Evidence for the close interaction is found in a tentative warp of 6,deg in the inner 3,au of the disk of RW,Aur,A, in the brightness temperature of both disks, and in the morphology of the gas emission. A narrow ring that peaks at 6,au around RW,Aur,B is suggestive of captured material from the disk around RW,Aur,A.
{"title":"Binary orbit and disks properties of the RW Aur system using ALMA observations","authors":"N. Kurtovic, S. Facchini, M. Benisty, P. Pinilla, S. Cabrit, E.L.N. Jensen, C. Dougados, R. Booth, C. N. Kimmig, C. Manara, J. E. Rodriguez","doi":"10.1051/0004-6361/202347583","DOIUrl":"https://doi.org/10.1051/0004-6361/202347583","url":null,"abstract":"The dynamical interactions between young binaries can perturb the material distribution of their circumstellar disks, and modify the planet formation process. In order to understand how planets form in multiple stellar systems, it is necessary to characterize both their binary orbit and their disks properties. In order to constrain the impact and nature of the binary interaction in the RW,Aur system (bound or unbound), we analyzed the circumstellar material at 1.3,mm wavelengths, as observed at multiple epochs by the Atacama Large (sub-)millimeter Array (ALMA). We analyzed the disk properties through parametric visibility modeling, and we used this information to constrain the dust morphology and the binary orbital period. We imaged the dust continuum emission of RW,Aur with a resolution of 3,au, and we find that the radius enclosing 90 of the flux 90 $) is 19,au and 14,au for RW,Aur,A and B, respectively. By modeling the relative distance of the disks at each epoch, we find a consistent trend of movement for the disk of RW,Aur,B moving away from the disk of RW,Aur,A at an approximate rate of $ in sky-projected distance). \u0000 By combining ALMA astrometry, historical astrometry, and the dynamical masses of each star, we constrain the RW,Aur binary stars to be most likely in a high-eccentricity elliptical orbit with a clockwise prograde orientation relative to RW,Aur,A, although low-eccentricity hyperbolic orbits are not ruled out by the astrometry. Our analysis does not exclude the possibility of a disk collision during the last interaction, which occurred $,yr ago relative to beginning of 2024. Evidence for the close interaction is found in a tentative warp of 6,deg in the inner 3,au of the disk of RW,Aur,A, in the brightness temperature of both disks, and in the morphology of the gas emission. A narrow ring that peaks at 6,au around RW,Aur,B is suggestive of captured material from the disk around RW,Aur,A.","PeriodicalId":8585,"journal":{"name":"Astronomy & Astrophysics","volume":"12 2","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-07-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141802093","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 : 2024-07-26DOI: 10.1051/0004-6361/202449861
Mikko Tuomi, J. Jyri Lehtinen, W. Gregory Henry, T. Hackman
Stellar spot distribution has consequences on the observable periodic signals in long-time baseline ground-based photometry. We model the statistics of the dominating spots of two young and active Solar-type stars, V889 Her and LQ Hya, in order to obtain information on the underlying spot distribution, rotation of the star, as well as the orientation of the stellar axis of spin. By calculating estimates for spot-induced periodicities in independent subsets of photometric data, we obtain statistics based on the dominating spots in each subset, giving rise to largest-spot statistics accounting for stellar geometry and rotation, including differential rotation. Our simple statistical models are able to reproduce the observed distribution of photometric signals rather well. This also enables us to estimate the dependence of angular velocity of the spots as a function of latitude. Our results indicate that V889 Her has a non-monotonic differential rotation curve with a maximum angular velocity between latitudes of 37-40 deg and lower angular velocity at the pole than the equator. Our results for LQ Hya indicate that the star rotates much like a rigid body. Furthermore, the results imply that the monotonic Solar differential rotation curve may not be a universal model for other solar-type stars. The non-monotonicity of the differential rotation of V889 Her is commonly produced in magnetohydrodynamic simulations, which indicates that our results are realistic from a theoretical perspective.
恒星光斑分布对长基线地基光度测量中可观测到的周期信号有影响。我们对两颗年轻而活跃的太阳型恒星--V889 Her 和 LQ Hya--的主要星斑的统计数据进行建模,以获得关于基本星斑分布、恒星自转以及恒星自旋轴方向的信息。通过计算独立测光数据子集中的光斑诱导周期性估计值,我们获得了基于每个子集中主要光斑的统计数据,从而得出了考虑到恒星几何形状和自转(包括差转)的最大光斑统计数据。我们的简单统计模型能够很好地再现观测到的测光信号的分布。这也使我们能够估计光斑角速度与纬度的函数关系。我们的结果表明,V889 Her 具有一条非单调的差转曲线,其最大角速度在纬度 37-40 度之间,极地的角速度低于赤道。我们对 LQ Hya 的研究结果表明,这颗恒星的旋转很像一个刚体。此外,这些结果还表明,单调的太阳差分自转曲线可能并不是其他太阳型恒星的通用模型。V889 Her 星差分自转的非单调性在磁流体动力学模拟中很常见,这表明我们的结果从理论角度来看是符合实际的。
{"title":"Characterising the stellar differential rotation based on largest-spot statistics from ground-based photometry","authors":"Mikko Tuomi, J. Jyri Lehtinen, W. Gregory Henry, T. Hackman","doi":"10.1051/0004-6361/202449861","DOIUrl":"https://doi.org/10.1051/0004-6361/202449861","url":null,"abstract":"Stellar spot distribution has consequences on the observable periodic signals in long-time baseline ground-based photometry. We model the statistics of the dominating spots of two young and active Solar-type stars, V889 Her and LQ Hya, in order to obtain information on the underlying spot distribution, rotation of the star, as well as the orientation of the stellar axis of spin. By calculating estimates for spot-induced periodicities in independent subsets of photometric data, we obtain statistics based on the dominating spots in each subset, giving rise to largest-spot statistics accounting for stellar geometry and rotation, including differential rotation. Our simple statistical models are able to reproduce the observed distribution of photometric signals rather well. This also enables us to estimate the dependence of angular velocity of the spots as a function of latitude. Our results indicate that V889 Her has a non-monotonic differential rotation curve with a maximum angular velocity between latitudes of 37-40 deg and lower angular velocity at the pole than the equator. Our results for LQ Hya indicate that the star rotates much like a rigid body. Furthermore, the results imply that the monotonic Solar differential rotation curve may not be a universal model for other solar-type stars. The non-monotonicity of the differential rotation of V889 Her is commonly produced in magnetohydrodynamic simulations, which indicates that our results are realistic from a theoretical perspective.","PeriodicalId":8585,"journal":{"name":"Astronomy & Astrophysics","volume":"40 26","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-07-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141800205","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 : 2024-07-26DOI: 10.1051/0004-6361/202450453
T. Miyaji, B. Bravo-Navarro, J. Diaz Tello, M. Krumpe, M. Herrera-Endoqui, H. Ikeda, T. Takagi, N. Oi, A. Shogaki, S. Matsuura, H. Kim, M. Malkan, H. Hwang, T. Kim, T. Ishigaki, H. Hanami, S.J. Kim, Y. Ohyama, T. Goto, H. Matsuhara
We present a catalog of optical and infrared (NIR) identifications (ID) of X-ray sources in the AKARI North Ecliptic Pole (NEP) deep field detected with Chandra covering $ $ and with 0.5-2 keV flux limits ranging between $ The optical/NIR counterparts of the X-ray sources were taken from our Hyper Suprime Cam (HSC)/Subaru and Wide-Field InfraRed Camera (WIRCam)/Canada-France-Hawaii Telescope (CFHT) data because these have much more accurate source positions due to their spatial resolution than those of Chandra and longer wavelength IR data. We concentrate our identifications in the HSC $g$ band and WIRCam $K_ s $ band-based catalogs. To select the best counterpart, we utilized a novel extension of the likelihood-ratio (LR) analysis, where we used the X-ray flux as well as $g - K_ s $ colors to calculate the likelihood ratio. The spectroscopic and photometric redshifts of the counterparts are summarized in this work. In addition, simple X-ray spectroscopy was carried out on the sources with sufficient source counts. We present the resulting catalog in an electronic form. The main ID catalog contains 403 X-ray sources and includes X-ray fluxes luminosities $g$ and $K_ s $ band magnitudes, redshifts and their sources, and optical spectroscopic properties, as well as intrinsic absorption column densities and power-law indices from simple X-ray spectroscopy. The X-ray sources identified in this work include 27 Milky-Way objects, 57 type I AGNs, 131 other AGNs, and 15 galaxies. The catalog serves as a basis for further investigations of the properties of the X-ray and NIR sources in this field. We present a catalog of optical ($g$ band) and NIR ($K_ s $ band) identifications of Chandra X-ray sources in the AKARI NEP Deep field with available optical/NIR spectroscopic features and redshifts as well as the results of simple X-ray spectroscopy. In the process, we developed a novel X-ray flux-dependent likelihood-ratio analysis for selecting the most likely counterparts among candidates.
我们提供了用钱德拉探测到的AKARI北黄道极(NEP)深场X射线源的光学和红外(NIR)识别(ID)目录,其覆盖范围为$ $,0.X 射线源的光学/近红外对应数据来自我们的超级超级相机 (HSC)/Subaru 和宽视场红外相机 (WIRCam)/Canada-France-Hawaii Telescope (CFHT) 数据,因为这些数据的空间分辨率比钱德拉和长波长红外数据的空间分辨率更高更精确。我们的识别工作主要集中在基于 HSC $g$ 波段和 WIRCam $K_ s$ 波段的星表中。为了选择最佳的对应天体,我们使用了似然比(LR)分析的新扩展方法,即使用X射线通量以及g - K_ s $颜色来计算似然比。这项工作总结了对应天体的光谱和光度红移。此外,我们还对有足够源计数的天体进行了简单的 X 射线光谱分析。我们以电子版的形式展示了所得到的星表。主 ID 星表包含 403 个 X 射线源,包括 X 射线通量光度 $g$ 和 $K_ s $ 波段星等、红移及其来源、光学光谱特性,以及简单 X 射线光谱分析得出的本征吸收柱密度和幂律指数。这项工作中确定的 X 射线源包括 27 个银河系天体、57 个 I 型 AGN、131 个其他 AGN 和 15 个星系。该星表为进一步研究该领域的 X 射线和近红外源的性质奠定了基础。我们提供了 AKARI NEP 深场中钱德拉 X 射线源的光学($g$波段)和近红外($K_ s$波段)识别目录,其中包括现有的光学/近红外光谱特征和红移,以及简单的 X 射线光谱分析结果。在此过程中,我们开发了一种新的 X 射线通量相关似然比分析方法,用于从候选天体中选择最有可能的对应天体。
{"title":"Chandra Survey in the AKARI deep field at the North Ecliptic Pole. Optical and near-infrared identifications of X-ray sources","authors":"T. Miyaji, B. Bravo-Navarro, J. Diaz Tello, M. Krumpe, M. Herrera-Endoqui, H. Ikeda, T. Takagi, N. Oi, A. Shogaki, S. Matsuura, H. Kim, M. Malkan, H. Hwang, T. Kim, T. Ishigaki, H. Hanami, S.J. Kim, Y. Ohyama, T. Goto, H. Matsuhara","doi":"10.1051/0004-6361/202450453","DOIUrl":"https://doi.org/10.1051/0004-6361/202450453","url":null,"abstract":"We present a catalog of optical and infrared (NIR) identifications (ID) of X-ray sources in the AKARI North Ecliptic Pole (NEP) deep field detected with Chandra covering $ $ and with 0.5-2 keV flux limits ranging between $ The optical/NIR counterparts of the X-ray sources were taken from our Hyper Suprime Cam (HSC)/Subaru and Wide-Field InfraRed Camera (WIRCam)/Canada-France-Hawaii Telescope (CFHT) data because these have much more accurate source positions due to their spatial resolution than those of Chandra and longer wavelength IR data. We concentrate our identifications in the HSC $g$ band and WIRCam $K_ s $ band-based catalogs. To select the best counterpart, we utilized a novel extension of the likelihood-ratio (LR) analysis, where we used the X-ray flux as well as $g - K_ s $ colors to calculate the likelihood ratio. The spectroscopic and photometric redshifts of the counterparts are summarized in this work. In addition, simple X-ray spectroscopy was carried out on the sources with sufficient source counts. We present the resulting catalog in an electronic form. The main ID catalog contains 403 X-ray sources and includes X-ray fluxes luminosities $g$ and $K_ s $ band magnitudes, redshifts and their sources, and optical spectroscopic properties, as well as intrinsic absorption column densities and power-law indices from simple X-ray spectroscopy. The X-ray sources identified in this work include 27 Milky-Way objects, 57 type I AGNs, 131 other AGNs, and 15 galaxies. The catalog serves as a basis for further investigations of the properties of the X-ray and NIR sources in this field. We present a catalog of optical ($g$ band) and NIR ($K_ s $ band) identifications of Chandra X-ray sources in the AKARI NEP Deep field with available optical/NIR spectroscopic features and redshifts as well as the results of simple X-ray spectroscopy. In the process, we developed a novel X-ray flux-dependent likelihood-ratio analysis for selecting the most likely counterparts among candidates.","PeriodicalId":8585,"journal":{"name":"Astronomy & Astrophysics","volume":"39 18","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-07-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141800225","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 : 2024-07-26DOI: 10.1051/0004-6361/202450444
B. Patricelli, M. Bernardini, M. Ferro
Fast radio bursts (FRBs) are highly energetic radio transients with a duration of some milliseconds. Their physical origin is still unknown. Many models consider magnetars as possible FRB sources, which is supported by the observational association of FRBs with the galactic magnetar SGR 1935+2154. Magnetars are also thought to be the source of the power of a fraction of gamma-ray bursts (GRBs), which means that the two extreme phenomena might have a common progenitor. We placed constrains on this hypothesis by searching for possible associations between GRBs and FRBs with currently available catalogues and by estimating whether an association can be ruled out based on the lack of a coincident detection. We cross-matched all the Neil Gehrels Swift Observatory (Swift) GRBs detected so far with all the well-localised FRBs reported in the FRBSTATS catalogue, and we looked for FRB-GRB associations considering both spatial and temporal constraints. We also simulated a synthetic population of FRBs associated with Swift GRBs to estimate how likely a joint detection with current and future radio facilities is. We recovered two low-significance possible associations that were reported before from a match of the catalogues: GRB 110715A/FRB 20171209A and GRB 060502B/FRB 20190309A. However, our study shows that based on the absence of any unambiguous association so far between Swift GRBs and FRBs, we cannot exclude that the two populations are connected because of the characteristics of current GRB and FRB detectors. Currently available observational data are not sufficient to clearly exclude or confirm whether GRBs and FRBs are physically associated. In the next decade, the probability of detecting joint GRB-FRB events will be higher with new generations of GRB and FRB detectors, if any: future observations will therefore be key to placing more stringent constraints on the hypothesis that FRBs and GRBs have common progenitors.
快速射电暴(FRBs)是一种持续时间约为几毫秒的高能瞬变射电现象。它们的物理起源仍是未知的。许多模型都认为磁星可能是快速射电暴的来源,而观测到的快速射电暴与银河系磁星 SGR 1935+2154 的联系也证明了这一点。磁星也被认为是一部分伽马射线暴(GRBs)的能量来源,这意味着这两种极端现象可能有共同的起源。我们对这一假设进行了限制,利用现有的星表搜索伽马射线暴和 FRB 之间可能存在的联系,并估计是否可以根据缺乏重合探测来排除这种联系。我们将迄今为止探测到的所有 Neil Gehrels Swift 天文台(Swift)GRB 与 FRBSTATS 目录中报告的所有定位良好的 FRB 进行了交叉匹配,并在考虑空间和时间限制的情况下寻找 FRB-GRB 关联。我们还模拟了一个与 Swift GRB 相关的 FRB 合成群,以估计利用当前和未来的射电设施进行联合探测的可能性有多大。我们从星表的比对中恢复了两个低意义的可能关联:GRB 110715A/FRB 20171209A 和 GRB 060502B/FRB 20190309A。然而,我们的研究表明,基于迄今为止 Swift GRB 和 FRB 之间还没有任何明确的联系,我们不能排除这两个族群之间由于当前 GRB 和 FRB 探测器的特性而存在联系。目前可用的观测数据还不足以明确排除或确认 GRB 和 FRB 是否存在物理联系。在未来的十年中,如果有新一代的 GRB 和 FRB 探测器的话,探测到 GRB-FRB 联合事件的概率将会更高:因此,未来的观测将是对 FRB 和 GRB 具有共同祖先这一假说施加更严格限制的关键。
{"title":"Constraints on fast radio burst emission in the aftermath of gamma-ray bursts","authors":"B. Patricelli, M. Bernardini, M. Ferro","doi":"10.1051/0004-6361/202450444","DOIUrl":"https://doi.org/10.1051/0004-6361/202450444","url":null,"abstract":"Fast radio bursts (FRBs) are highly energetic radio transients with a duration of some milliseconds. Their physical origin is still unknown. Many models consider magnetars as possible FRB sources, which is supported by the observational association of FRBs with the galactic magnetar SGR 1935+2154. Magnetars are also thought to be the source of the power of a fraction of gamma-ray bursts (GRBs), which means that the two extreme phenomena might have a common progenitor. We placed constrains on this hypothesis by searching for possible associations between GRBs and FRBs with currently available catalogues and by estimating whether an association can be ruled out based on the lack of a coincident detection. We cross-matched all the Neil Gehrels Swift Observatory (Swift) GRBs detected so far with all the well-localised FRBs reported in the FRBSTATS catalogue, and we looked for FRB-GRB associations considering both spatial and temporal constraints. We also simulated a synthetic population of FRBs associated with Swift GRBs to estimate how likely a joint detection with current and future radio facilities is. We recovered two low-significance possible associations that were reported before from a match of the catalogues: GRB 110715A/FRB 20171209A and GRB 060502B/FRB 20190309A. However, our study shows that based on the absence of any unambiguous association so far between Swift GRBs and FRBs, we cannot exclude that the two populations are connected because of the characteristics of current GRB and FRB detectors. Currently available observational data are not sufficient to clearly exclude or confirm whether GRBs and FRBs are physically associated. In the next decade, the probability of detecting joint GRB-FRB events will be higher with new generations of GRB and FRB detectors, if any: future observations will therefore be key to placing more stringent constraints on the hypothesis that FRBs and GRBs have common progenitors.","PeriodicalId":8585,"journal":{"name":"Astronomy & Astrophysics","volume":"22 2","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-07-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141801658","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 : 2024-07-26DOI: 10.1051/0004-6361/202450532
M. Broz, P. Vernazza, M. Marsset, R. Binzel, F. DeMeo, M. Birlan, F. Colas, S. Anghel, S. Bouley, C. Blanpain, J. Gattacceca, S. Jeanne, L. Jorda, J. Lecubin, A. Malgoyre, A. Steinhausser, J. Vaubaillon, B. Zanda
The source regions of ordinary chondrites (sim 80 of all falls) and large S-type near-Earth objects (NEOs; sim 30) have recently been identified with three young asteroid families (Karin, Koronis, Massalia) being at the origin of most ordinary chondrite falls. The present work is a continuation of our previous studies and aims to determine the source regions of the remaining meteorite and NEO classes, with an emphasis on carbonaceous chondrites (CM, CI, CO, CV, CK, CR, CH, CB, or C-ungrouped). We studied 38 individual asteroid families, including young and old ones, and determined their contributions to the NEO populations at metre and kilometre sizes using collisional and orbital models. Our models are in agreement with spectroscopic observations of NEOs, cosmic-ray exposure ages of meteorites, statistics of bolides, infrared emission from dust bands, composition of interplanetary dust particles (IDPs), and abundance of extraterrestrial helium-3. We identified the Veritas, Polana, and Eos families as the primary sources of CM/CR, CI, and CO/CV/CK chondrites, respectively. Substantial contributions are also expected from CM-like K"onig and CI-like Clarissa, Misa, and Hoffmeister families. The source regions of kilometre-sized bodies are generally different. The Adeona family is by far the main source of CM-like NEOs, whereas the Polana (low-i) and Euphrosyne (high-i) families are at the origin of most CI-like NEOs. The Polana family is the likely source of both Ryugu and Bennu. We were able to link spectroscopically and dynamically several NEOs to the Baptistina family. Finally, it appears that the pre-atmospheric flux of carbonaceous chondrites at metre sizes is about the same as that of ordinary chondrites. Given the difference in fall statistics between the two groups (80 versus 4.4), this implies either substantial atmospheric fragmentation of carbonaceous bodies at the level of sim MPa $ or destruction by thermal cracking and water desorption. The source regions of most meteorites and kilometre-sized NEOs have now been determined, including some minor classes such as enstatite chondrites and achondrites (Nysa, Hungaria), acapulcoites and lodranites (Iannini). Future work should focus on the few remaining classes (essentially, iron meteorites, pallasites, and ureilites).
{"title":"Source regions of carbonaceous meteorites and near-Earth objects","authors":"M. Broz, P. Vernazza, M. Marsset, R. Binzel, F. DeMeo, M. Birlan, F. Colas, S. Anghel, S. Bouley, C. Blanpain, J. Gattacceca, S. Jeanne, L. Jorda, J. Lecubin, A. Malgoyre, A. Steinhausser, J. Vaubaillon, B. Zanda","doi":"10.1051/0004-6361/202450532","DOIUrl":"https://doi.org/10.1051/0004-6361/202450532","url":null,"abstract":"The source regions of ordinary chondrites (sim 80 of all falls)\u0000and large S-type near-Earth objects (NEOs; sim 30)\u0000have recently been identified\u0000with three young asteroid families (Karin, Koronis, Massalia)\u0000being at the origin of most ordinary chondrite falls. The present work is a continuation of our previous studies\u0000and aims to determine the source regions of the remaining meteorite and NEO classes,\u0000with an emphasis on carbonaceous chondrites\u0000(CM, CI, CO, CV, CK, CR, CH, CB, or C-ungrouped). We studied 38 individual asteroid families, including young and old ones,\u0000and determined their contributions to the NEO populations at metre and kilometre sizes\u0000using collisional and orbital models.\u0000Our models are in agreement with\u0000spectroscopic observations of NEOs,\u0000cosmic-ray exposure ages of meteorites,\u0000statistics of bolides,\u0000infrared emission from dust bands,\u0000composition of interplanetary dust particles (IDPs), and\u0000abundance of extraterrestrial helium-3. We identified the Veritas, Polana, and Eos families\u0000as the primary sources of CM/CR, CI, and CO/CV/CK chondrites, respectively.\u0000Substantial contributions are also expected from\u0000CM-like K\"onig and CI-like Clarissa, Misa, and Hoffmeister families. The source regions of kilometre-sized bodies are generally different. The Adeona family is by far the main source of CM-like NEOs, whereas the Polana (low-i) and Euphrosyne (high-i) families are at the origin of most CI-like NEOs. The Polana family is the likely source of both Ryugu and Bennu. We were able to link spectroscopically and dynamically several NEOs to the Baptistina family. Finally, it appears that the pre-atmospheric flux of carbonaceous chondrites at metre sizes is about the same as that of ordinary chondrites. Given the difference in fall statistics between the two groups (80 versus 4.4), this implies either substantial atmospheric fragmentation of carbonaceous bodies at the level of sim MPa $\u0000or destruction by thermal cracking and water desorption. The source regions of most meteorites and kilometre-sized NEOs have now been determined,\u0000including some minor classes such as\u0000enstatite chondrites and achondrites (Nysa, Hungaria),\u0000acapulcoites and lodranites (Iannini).\u0000Future work should focus on the few remaining classes (essentially, iron meteorites, pallasites, and ureilites).","PeriodicalId":8585,"journal":{"name":"Astronomy & Astrophysics","volume":"36 50","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-07-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141800373","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 : 2024-07-26DOI: 10.1051/0004-6361/202451113
A. Traina, B. Magnelli, C. Gruppioni, I. Delvecchio, M. Parente, F. Calura, L. Bisigello, A. Feltre, F. Pozzi, L. Vallini
Although dust in galaxies represents only a few percent of the total baryonic mass, it plays a crucial role in the physical processes occurring in galaxies. Studying the dust content of galaxies, particularly at high $z$, is therefore crucial for understanding the link between dust production, obscured star formation, and the build-up of galaxy stellar mass. We study the dust properties (mass and temperature) of the largest Atacama Large Millimeter/submillimeter Array (ALMA)-selected sample of star-forming galaxies available from the archive (A$^3$COSMOS), and we derive the dust mass function and dust mass density of galaxies from $z=0.5,-,6$. We fit the spectral energy distribution (SED) with the CIGALE code to constrain the dust mass and temperature of the A$^3$COSMOS galaxy sample based on the UV-to-near-infrared photometric coverage of each galaxy combined with the ALMA (and Herschel when available) coverage of the Rayleigh-Jeans tail of their dust-continuum emission. We then computed and fit the dust mass function by combining the A$^3$COSMOS and the most recent Herschel samples in order to obtain the best estimate of the integrated dust mass density up to $z The dust masses in galaxies in lie between $ 10^8$ and $ $ M$_ odot $. From the SED fitting, we were also able to derive a dust temperature. The distribution of the dust temperature peaks at $ 30-35$K. The dust mass function at $z=0.5,-,6$ evolves with an increase in $M^*$ and a decrease in the number density ($ ^*$), and it agrees well with literature estimates. The dust mass density decreases smoothly in its evolution from $z 0.5$ to $z 6$, which is steeper than what is found by models at $z
{"title":"A^3COSMOS: Dust mass function and dust mass density at 0.5","authors":"A. Traina, B. Magnelli, C. Gruppioni, I. Delvecchio, M. Parente, F. Calura, L. Bisigello, A. Feltre, F. Pozzi, L. Vallini","doi":"10.1051/0004-6361/202451113","DOIUrl":"https://doi.org/10.1051/0004-6361/202451113","url":null,"abstract":"Although dust in galaxies represents only a few percent of the total baryonic mass, it plays a crucial role in the physical processes occurring in galaxies. Studying the dust content of galaxies, particularly at high $z$, is therefore crucial for understanding the link between dust production, obscured star formation, and the build-up of galaxy stellar mass. We study the dust properties (mass and temperature) of the largest Atacama Large Millimeter/submillimeter Array (ALMA)-selected sample of star-forming galaxies available from the archive (A$^3$COSMOS), and we derive the dust mass function and dust mass density of galaxies from $z=0.5,-,6$. We fit the spectral energy distribution (SED) with the CIGALE code to constrain the dust mass and temperature of the A$^3$COSMOS galaxy sample based on the UV-to-near-infrared photometric coverage of each galaxy combined with the ALMA (and Herschel when available) coverage of the Rayleigh-Jeans tail of their dust-continuum emission. We then computed and fit the dust mass function by combining the A$^3$COSMOS and the most recent Herschel samples in order to obtain the best estimate of the integrated dust mass density up to $z The dust masses in galaxies in lie between $ 10^8$ and $ $ M$_ odot $. From the SED fitting, we were also able to derive a dust temperature. The distribution of the dust temperature peaks at $ 30-35$K. The dust mass function at $z=0.5,-,6$ evolves with an increase in $M^*$ and a decrease in the number density ($ ^*$), and it agrees well with literature estimates. The dust mass density decreases smoothly in its evolution from $z 0.5$ to $z 6$, which is steeper than what is found by models at $z","PeriodicalId":8585,"journal":{"name":"Astronomy & Astrophysics","volume":"50 9","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-07-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141798952","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-07-26DOI: 10.1051/0004-6361/202142892
Barbara Mazzilli Ciraulo, A. Melchior, F. Combes, Daniel Maschmann
Understanding the relationship between quenching mechanisms that transform star-forming galaxies into quiescent ones and galaxy properties remains a challenge. We investigate the gas and stellar properties of 69 double-peaked galaxies selected from the Sloan Digital Sky Survey (SDSS) and observed as part of the Mapping Nearby Galaxies at APO (MaNGA) survey to elucidate the mechanisms driving star formation quenching within these systems. We study their star formation activity along with their physical properties: colour, morphology, environment, stellar age, and gas ionisation diagnostics. We find that these 69 double-peaked MaNGA galaxies encompass a higher fraction of galaxies in the green valley, based on the corrected NUV-$r$ colour, compared to our defined control samples of single-peaked emission line galaxies. This green colour traces intermediate stellar populations compared to blue and red galaxies, as indicated by the D$_n(4000)$ index. These green galaxies show no recent star formation bursts within the last 2 Gyr. They exhibit emission line ratios that are suggestive of both ongoing star formation and nuclear activity. They are predominantly located in isolated or small group environments, indicating that internal processes rather than external factors drive their quenching. Moreover, optical emission lines detected throughout a significant area of these systems suggest that gas depletion is unlikely to be the primary quenching mechanism. These findings support a scenario where quenching is instead caused by reduced star formation efficiency.
了解将恒星形成星系转变为静止星系的淬火机制与星系特性之间的关系仍然是一个挑战。我们研究了从斯隆数字巡天(SDSS)中选取的69个双峰星系的气体和恒星特性,这些星系是在Mapping Nearby Galaxies at APO(MaNGA)巡天中观测到的,目的是阐明这些星系中恒星形成淬火的驱动机制。我们研究了它们的恒星形成活动及其物理性质:颜色、形态、环境、恒星年龄和气体电离诊断。我们发现,与我们定义的单峰发射线星系对照样本相比,根据校正后的 NUV-$r$ 颜色,这 69 个双峰 MaNGA 星系包含了更高比例的绿谷星系。根据 D$_n(4000)$ 指数显示,与蓝色和红色星系相比,绿色星系的恒星数量处于中等水平。这些绿色星系在过去的 2 Gyr 内没有出现新的恒星形成爆发。它们的发射线比率表明恒星形成和核活动都在进行中。它们主要位于孤立或小星系群环境中,表明是内部过程而不是外部因素导致了它们的熄灭。此外,在这些系统的相当大的范围内探测到的光学发射线表明,气体耗竭不太可能是主要的淬火机制。这些发现支持恒星形成效率降低导致熄灭的观点。
{"title":"Resolving double-peaked emission line galaxies using MaNGA. I. Mechanisms of star formation quenching","authors":"Barbara Mazzilli Ciraulo, A. Melchior, F. Combes, Daniel Maschmann","doi":"10.1051/0004-6361/202142892","DOIUrl":"https://doi.org/10.1051/0004-6361/202142892","url":null,"abstract":"Understanding the relationship between quenching mechanisms that transform star-forming galaxies into quiescent ones and galaxy properties remains a challenge. \u0000\u0000We investigate the gas and stellar properties of 69 double-peaked galaxies selected from the Sloan Digital Sky Survey (SDSS) and observed as part of the Mapping Nearby Galaxies at APO (MaNGA) survey to elucidate the mechanisms driving star formation quenching within these systems. We study their star formation activity along with their physical properties: colour, morphology, environment, stellar age, and gas ionisation diagnostics. \u0000We find that these 69 double-peaked MaNGA galaxies encompass a higher fraction of galaxies in the green valley, based on the corrected NUV-$r$ colour, compared to our defined control samples of single-peaked emission line galaxies. This green colour traces intermediate stellar populations compared to blue and red galaxies, as indicated by the D$_n(4000)$ index. These green galaxies show no recent star formation bursts within the last 2 Gyr. They exhibit emission line ratios that are suggestive of both ongoing star formation and nuclear activity. They are predominantly located in isolated or small group environments, indicating that internal processes rather than external factors drive their quenching. Moreover, optical emission lines detected throughout a significant area of these systems suggest that gas depletion is unlikely to be the primary quenching mechanism. These findings support a scenario where quenching is instead caused by reduced star formation efficiency.","PeriodicalId":8585,"journal":{"name":"Astronomy & Astrophysics","volume":"30 8","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-07-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141800920","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}