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Pulsation modes of three Delta Scuti stars using Kepler project data: KIC3429637, KIC10451090, KIC2987660 利用开普勒项目数据研究三颗德尔塔苏蒂星的脉动模式:KIC3429637、KIC10451090、KIC2987660
IF 1.9 4区 物理与天体物理 Q2 ASTRONOMY & ASTROPHYSICS Pub Date : 2024-08-14 DOI: 10.1016/j.newast.2024.102294
Amin Shafaeiyeh Hiagh, Nematollah Riazi

We have analyzed the light curves of three δ Scuti stars that were observed by the Kepler Space Telescope. Data collected by the Kepler space telescope, as well as analysis of the light curve of each star and the use of online databases, have been utilized to achieve the objectives of this project. Data has been collected through Kepler's main mission. We compare both data that we get from the Lightkurve package of Python and the KASOC online data centre to verify the data. We select the necessary data like flux, observation date, and the spectral type of the stars. By investigating various types of pulsating variable stars, three Delta Scuti stars have been selected due to their flux, pulsating type, etc. It is observed that most of these stars are pulsating in the p-modes. However, the selected stars pulsate in both p-modes and (possibly) g-modes. We select these stars, due to the lack of articles about them. Furthermore, some physical properties of these stars are deduced from their light curves. In summary, the results of this study indicate that the stars KIC3429637 and KIC10451090 are pulsating only in p-modes, while KIC2987660 is pulsating both in p-modes and g-modes.

我们分析了开普勒太空望远镜观测到的三颗δ Scuti 星的光变曲线。开普勒太空望远镜收集的数据,以及对每颗恒星的光变曲线的分析和在线数据库的使用,都被用来实现本项目的目标。数据是通过开普勒的主要任务收集的。我们比较了从 Python 的 Lightkurve 软件包和 KASOC 在线数据中心获得的数据,以验证数据。我们选择必要的数据,如恒星的通量、观测日期和光谱类型。通过研究各种类型的脉动变星,根据它们的通量、脉动类型等,我们选出了三颗德尔塔Scuti星。据观察,这些恒星大多以 p 模式脉动。然而,被选中的恒星同时以 p 模式和(可能)g 模式脉动。我们选择这些恒星,是因为缺乏有关它们的文章。此外,我们还从这些恒星的光变曲线中推断出了它们的一些物理特性。总之,这项研究的结果表明,KIC3429637 和 KIC10451090 这两颗恒星只以 p 模式脉动,而 KIC2987660 则同时以 p 模式和 g 模式脉动。
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引用次数: 0
Combined light curve and radial velocity analysis of the neglected contact binary S Ant 被忽视的接触双星 S Ant 的综合光变曲线和径向速度分析
IF 1.9 4区 物理与天体物理 Q2 ASTRONOMY & ASTROPHYSICS Pub Date : 2024-08-12 DOI: 10.1016/j.newast.2024.102291
Olivera Latković, Atila Čeki

We present the first combined photometric and spectroscopic solution of the bright southern contact binary S Ant based on the Transiting Exoplanet Survey Satellite (TESS) light curve and the radial velocities from the David Dunlap Observatory survey. S Ant is a W UMa type binary in deep contact, with a mass ratio of 0.34 and a relatively massive and hot F-type primary. Beside the standard modeling of the phase-binned light curve, we also perform “seasonal modeling” where we treat each of the 83 orbital cycles present in the TESS data as a separate light curve. The resulting ensemble of solutions shows evidence of quasi-periodic migration of a long-lived, dark, polar spot. The migration is confirmed independently by eclipse time variations which display remarkably strong correlation with the spot location.

我们根据凌日系外行星巡天卫星(TESS)的光曲线和戴维-邓拉普天文台(David Dunlap Observatory)巡天观测的径向速度,首次提出了明亮的南方接触双星S Ant的光度和光谱综合解法。S Ant是一颗深度接触的W UMa型双星,质量比为0.34,主星质量相对较大,温度较高,属于F型。除了对相位分档光曲线进行标准建模外,我们还进行了 "季节建模",将 TESS 数据中的 83 个轨道周期中的每个周期都视为一条单独的光曲线。结果显示,有证据表明一个寿命较长的极地黑斑发生了准周期性迁移。日食时间的变化独立地证实了这种迁移,日食时间的变化与光斑位置显示出极强的相关性。
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引用次数: 0
The size and shape dependence of the SDSS galaxy bispectrum SDSS星系双谱的大小和形状依赖性
IF 1.9 4区 物理与天体物理 Q2 ASTRONOMY & ASTROPHYSICS Pub Date : 2024-08-10 DOI: 10.1016/j.newast.2024.102292
Anindita Nandi , Sukhdeep Singh Gill , Debanjan Sarkar , Abinash Kumar Shaw , Biswajit Pandey , Somnath Bharadwaj
<div><p>We have measured the spherically averaged bispectrum of the SDSS main galaxy sample, considering a volume-limited <span><math><msup><mrow><mrow><mo>[</mo><mn>296</mn><mo>.</mo><mn>75</mn><mspace></mspace><mi>Mpc</mi><mo>]</mo></mrow></mrow><mrow><mn>3</mn></mrow></msup></math></span> data cube with mean galaxy number density <span><math><mrow><mn>0</mn><mo>.</mo><mn>63</mn><mo>×</mo><msup><mrow><mn>10</mn></mrow><mrow><mo>−</mo><mn>3</mn></mrow></msup><mspace></mspace><msup><mrow><mi>Mpc</mi></mrow><mrow><mo>−</mo><mn>3</mn></mrow></msup></mrow></math></span> and median redshift <span><math><mrow><mn>0</mn><mo>.</mo><mn>102</mn></mrow></math></span>. Our analysis considers <span><math><mrow><mo>∼</mo><mn>1</mn><mo>.</mo><mn>37</mn><mo>×</mo><mn>1</mn><msup><mrow><mn>0</mn></mrow><mrow><mn>8</mn></mrow></msup></mrow></math></span> triangles, for which we have measured the binned bispectrum and analysed its dependence on the size and shape of the triangle. It spans wavenumbers <span><math><mrow><msub><mrow><mi>k</mi></mrow><mrow><mn>1</mn></mrow></msub><mo>=</mo><mrow><mo>(</mo><mn>0</mn><mo>.</mo><mn>075</mn><mo>−</mo><mn>0</mn><mo>.</mo><mn>434</mn><mo>)</mo></mrow><mspace></mspace><msup><mrow><mi>Mpc</mi></mrow><mrow><mo>−</mo><mn>1</mn></mrow></msup></mrow></math></span> for equilateral triangles, and a smaller range of <span><math><msub><mrow><mi>k</mi></mrow><mrow><mn>1</mn></mrow></msub></math></span> (the largest side) for triangles of other shapes. For all shapes, we find that the measured bispectrum is well modelled by a power law <span><math><mrow><mi>A</mi><mspace></mspace><msup><mrow><mrow><mo>(</mo><mrow><msub><mrow><mi>k</mi></mrow><mrow><mn>1</mn></mrow></msub><mo>/</mo><mn>1</mn><mspace></mspace><msup><mrow><mi>Mpc</mi></mrow><mrow><mo>−</mo><mn>1</mn></mrow></msup></mrow><mo>)</mo></mrow></mrow><mrow><mi>n</mi></mrow></msup></mrow></math></span>, where the best-fit values of <span><math><mi>A</mi></math></span> and <span><math><mi>n</mi></math></span> vary with the shape. The parameter <span><math><mi>A</mi></math></span> is the minimum for equilateral triangles and increases as the shape is deformed to linear triangles where the two largest sides are nearly aligned, reaching its maximum value for <span><math><mrow><mi>μ</mi><mo>=</mo><mn>0</mn><mo>.</mo><mn>95</mn><mo>,</mo><mspace></mspace><mi>t</mi><mo>=</mo><mn>0</mn><mo>.</mo><mn>75</mn></mrow></math></span>. The values of <span><math><mi>n</mi></math></span> are all negative, <span><math><mrow><mo>|</mo><mi>n</mi><mo>|</mo></mrow></math></span> is minimum <span><math><mrow><mo>(</mo><mn>3</mn><mo>.</mo><mn>12</mn><mo>±</mo><mn>0</mn><mo>.</mo><mn>35</mn><mo>)</mo></mrow></math></span> for the shape bin <span><math><mrow><mi>μ</mi><mo>=</mo><mn>0</mn><mo>.</mo><mn>65</mn><mo>,</mo><mspace></mspace><mi>t</mi><mo>=</mo><mn>0</mn><mo>.</mo><mn>75</mn></mrow></math></span>, and <span><math><mrow><mn>3</mn><mo>.</mo><mn>8</mn><mo>±</mo><mn>0</mn><mo>.</mo><mn>28</mn></mrow
我们测量了SDSS主星系样本的球形平均双谱,考虑了一个体积有限的[296.75Mpc]3数据立方体,其平均星系数密度为0.63×10-3Mpc-3,中位红移为0.102。我们的分析考虑了 ∼1.37×108 个三角形,测量了这些三角形的二分双谱,并分析了它与三角形大小和形状的关系。对于等边三角形,它的波数范围是 k1=(0.075-0.434)Mpc-1 ,对于其他形状的三角形,k1(最大边)的范围较小。我们发现,对于所有形状,测量到的双光谱都可以很好地用幂律 A(k1/1Mpc-1)n 来模拟,其中 A 和 n 的最佳拟合值随形状的变化而变化。参数 A 在等边三角形时最小,随着形状变形为最大两边几乎对齐的线性三角形而增大,在 μ=0.95,t=0.75 时达到最大值。n的值都是负数,μ=0.65,t=0.75时,n的值最小(3.12±0.35),μ=0.65,t=0.85时,n的值为3.8±0.28。我们还分析了根据ΛCDM N-body模拟构建的模拟星系样本,方法是应用一个简单的欧拉偏差处方,即星系位于平滑密度场超过阈值的区域。我们发现,在偏差 b1=1.2 的条件下,模拟样本的双谱与 SDSS 的结果非常吻合。我们进一步将星系样本分为红色和蓝色两类,并研究了每一类星系的双谱性质。在所有可能的三角形配置中,红色星系的双谱振幅A都高于蓝色星系。红色星系年代久远,它们的双光谱较大,这表明随着时间的推移,它们所处的环境发生了非线性的演化相互作用,导致它们的分布高度集群,比年轻的蓝色星系更有偏差。
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Our analysis considers &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mo&gt;∼&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;37&lt;/mn&gt;&lt;mo&gt;×&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;8&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt; triangles, for which we have measured the binned bispectrum and analysed its dependence on the size and shape of the triangle. It spans wavenumbers &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;k&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;075&lt;/mn&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;434&lt;/mn&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;Mpc&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt; for equilateral triangles, and a smaller range of &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;k&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt; (the largest side) for triangles of other shapes. For all shapes, we find that the measured bispectrum is well modelled by a power law &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mi&gt;A&lt;/mi&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mrow&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;k&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;/&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;Mpc&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/mrow&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt;, where the best-fit values of &lt;span&gt;&lt;math&gt;&lt;mi&gt;A&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt; and &lt;span&gt;&lt;math&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt; vary with the shape. The parameter &lt;span&gt;&lt;math&gt;&lt;mi&gt;A&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt; is the minimum for equilateral triangles and increases as the shape is deformed to linear triangles where the two largest sides are nearly aligned, reaching its maximum value for &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mi&gt;μ&lt;/mi&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;95&lt;/mn&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;75&lt;/mn&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt;. The values of &lt;span&gt;&lt;math&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt; are all negative, &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt; is minimum &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mn&gt;3&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;12&lt;/mn&gt;&lt;mo&gt;±&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;35&lt;/mn&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt; for the shape bin &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mi&gt;μ&lt;/mi&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;65&lt;/mn&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;75&lt;/mn&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt;, and &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mn&gt;3&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;8&lt;/mn&gt;&lt;mo&gt;±&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;28&lt;/mn&gt;&lt;/mrow","PeriodicalId":54727,"journal":{"name":"New Astronomy","volume":"113 ","pages":"Article 102292"},"PeriodicalIF":1.9,"publicationDate":"2024-08-10","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142006419","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
Asteroseismology of evolved stars in six star clusters observed by Kepler/K2 开普勒/K2观测到的六个星团中的演化恒星的小行星动力学
IF 1.9 4区 物理与天体物理 Q2 ASTRONOMY & ASTROPHYSICS Pub Date : 2024-07-27 DOI: 10.1016/j.newast.2024.102290
Yun-A Jo, Heon-Young Chang

In this study, we have explored the frequency separations, Δν and δν02, the height and width of the oscillation power excess, HGauss and δνenv, as a function of the frequency of maximum power νmax by analyzing 187 evolved stars in six star clusters observed by the Kepler/K2 missions. We have also examined the asteroseismic relation in the Christensen-Dalsgaard diagram. Given the importance of scaling relations, the dependency of asteroseismic scaling relations on physical quantities must be verified to reduce systematic errors through the exploration of observational data obtained from various sources. In this context, the star cluster provides a valuable means to assess the age and metallicity. Focusing on evolved stars with 30μHz<νmax<220μHz, we have exploited the mass effect without the need for deriving the individual stellar mass. We have found that the considered relations appear to be associated with the age of star clusters, thereby the mass of the stars in a given evolutionary status for star clusters with different ages. By separately considering red giant branch stars and red clump stars, we have found that red clump stars appear more sensitive to the cluster age compared with red giant branch stars. It has been suggested that conclusions regarding the dependency of metallicity should be drawn with due care as outcomes are subject to how to treat metallicity. Finally, we conclude by briefly pointing out implications of our findings on asteroseismic inferences.

在这项研究中,我们通过分析开普勒/K2任务观测到的6个星团中的187颗演化星,探讨了频率间隔Δν和δν02、振荡功率过度的高度和宽度HGauss和δνenv与最大功率频率νmax的函数关系。我们还研究了克里斯滕森-达尔斯加尔德图中的星震关系。鉴于缩放关系的重要性,必须通过探索从各种来源获得的观测数据来验证星震缩放关系对物理量的依赖性,以减少系统误差。在这种情况下,星团为评估年龄和金属性提供了宝贵的手段。我们以30μHz<νmax<220μHz的演化恒星为重点,利用了质量效应,而无需推导单个恒星的质量。我们发现,所考虑的关系似乎与星团的年龄有关,因此不同年龄的星团在特定演化状态下的恒星质量也不同。通过分别考虑红巨分支恒星和红团块恒星,我们发现与红巨分支恒星相比,红团块恒星似乎对星团年龄更加敏感。有人建议,在得出有关金属性依赖性的结论时应充分谨慎,因为结果取决于如何处理金属性。最后,我们简要地指出了我们的发现对小行星地震推断的影响。
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引用次数: 0
Further lunar occultations results from the Trebur Observatory, 2021–24 2021-24 年特雷伯天文台的进一步月掩结果
IF 1.9 4区 物理与天体物理 Q2 ASTRONOMY & ASTROPHYSICS Pub Date : 2024-07-27 DOI: 10.1016/j.newast.2024.102289
J.M. Ohlert , A. Richichi

Following up on our initial paper (Richichi and Ohlert, 2021), we report here on 60 lunar occultation events recorded between February 2021 and March 2024 at the Michael Adrian Observatorium. An improved version of the detector was employed for the present work. The program aims mainly at the direct measurement of the angular diameter of late-type stars, and the discovery or confirmation of binary stars with small separations. Among the results, we present first time angular diameter determinations for the late-type M giants IRC +20184 and BL Tau and for the bright carbon star TU Gem. Our diameter result for RX Cnc is the first determination outside the near-IR range. We also discovered or detected directly for the first time companions around SAO 79580, BL Tau again, and SAO 78643. The lunar occultation technique at our facility is capable to reach sources as faint as 10 V magnitude with an angular resolution at the milliarcsecond level.

继我们最初的论文(Richichi 和 Ohlert,2021 年)之后,我们在此报告 2021 年 2 月至 2024 年 3 月期间在迈克尔-阿德里安天文台记录的 60 次月球掩星事件。本次工作使用了改进版探测器。该计划的主要目的是直接测量晚期恒星的角直径,以及发现或确认小间隔双星。在这些成果中,我们首次测定了晚M型巨星IRC +20184和BL Tau以及明亮碳星TU Gem的角直径。我们对 RX Cnc 的直径测定结果是首次在近红外范围之外进行的。我们还首次发现或直接探测到了 SAO 79580、BL Tau 和 SAO 78643 周围的伴星。我们设施的月球掩星技术能够以毫厘秒级的角分辨率观测到≈10 V等的暗源。
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引用次数: 0
Wormholes in dwarf and spiral galactic halo regions 矮星系和螺旋星系晕区的虫洞
IF 1.9 4区 物理与天体物理 Q2 ASTRONOMY & ASTROPHYSICS Pub Date : 2024-07-20 DOI: 10.1016/j.newast.2024.102288
Mehedi Kalam , Amir Ghari , Irina Radinschi , Hosein Haghi , Farook Rahaman , Tandrima Chowdhury

In this article, we study solutions which describe wormholes in the halos of dwarf and massive spiral galaxies with different morphologies, masses, sizes and gas fractions by taking observed flat rotation curves as input. We assume Singular Isothermal Sphere (SIS) dark matter density profile. This result confirms the possible existence of wormholes in both dwarf and massive spiral galaxies.

在本文中,我们以观测到的平直旋转曲线为输入,研究了描述不同形态、质量、大小和气体比例的矮星系和大质量旋涡星系光晕中虫洞的解。我们假设暗物质密度曲线为奇异等温球(SIS)。这一结果证实了矮星系和大质量旋涡星系中都可能存在虫洞。
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引用次数: 0
Definition of multispectral camera system parameters to model the asteroid 2001 SN263 确定多光谱摄像系统参数以模拟小行星 2001 Sn263
IF 1.9 4区 物理与天体物理 Q2 ASTRONOMY & ASTROPHYSICS Pub Date : 2024-07-15 DOI: 10.1016/j.newast.2024.102287
Gabriela de Carvalho Assis Goulart , Thiago Statella , Rafael Sfair

In 2012, Brazil began the studies to send its first deep space exploration mission, ASTER, which would be the first mission to orbit a triple asteroid system, 2001 SN263. We aim to contribute to the ASTER mission by defining the parameters of a multispectral camera system that will be used to study the asteroid system 2001 SN263, through software simulations that should help planning the data collection. We inserted the shape model of the objects in the software POV-Ray and modeled two cameras, a Wide Angle (WAC) and a Narrow Angle (NAC). We inserted the asteroid's parameters and simulated the satellite position. We created various scenes so we could obtain a good view of the asteroid. Alpha is entirely visible only in the WAC images, while the NAC is expected to reveal surface details. Beta seems relatively small in the WAC images, whereas we obtain a broad view from the NAC at 100 km distance. Gamma, smaller than Beta, should provide more detailed images through the NAC, whereas the WAC images should be able to show its inclined orbit around Alpha. To see Gamma behind Alpha in its revolution movement, we would have to elevate the camera's orbit. The method employed to simulate images generated by satellite cameras can be applied to other scenarios where the target requires imaging, extending beyond the field of planetary geology.

2012年,巴西开始研究发送其首个深空探测任务ASTER,这将是首个绕三重小行星系统2001 SN263运行的任务。我们的目标是通过软件模拟,确定用于研究小行星系统 2001 SN263 的多光谱摄像系统的参数,从而为 ASTER 任务做出贡献。我们在 POV-Ray 软件中插入了天体的形状模型,并模拟了两台照相机,一台是广角(WAC),另一台是窄角(NAC)。我们插入了小行星的参数,并模拟了卫星的位置。我们创建了各种场景,以便获得小行星的良好视角。只有在 WAC 图像中才能完全看到 Alpha,而 NAC 预计能显示表面细节。在 WAC 图像中,Beta 似乎相对较小,而我们从距离 100 千米的 NAC 可以获得广阔的视野。伽马星比贝塔星小,通过 NAC 可以获得更详细的图像,而 WAC 图像则可以显示出它围绕阿尔法星的倾斜轨道。要想看到 Gamma 在 Alpha 后方的旋转运动,我们必须抬高照相机的轨道。模拟卫星照相机生成图像的方法可以应用于其他需要对目标成像的情况,而不仅仅局限于行星地质学领域。
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引用次数: 0
Modeling compact stars with two fluids 用两种流体模拟紧凑恒星
IF 1.9 4区 物理与天体物理 Q2 ASTRONOMY & ASTROPHYSICS Pub Date : 2024-07-11 DOI: 10.1016/j.newast.2024.102286
Pedro Mafa , Vishnu Kakkat , Amos Kubeka , Mantile Lekala

In this paper, we study the curved Krori–Barua spacetime geometry to describe compact stars with two components: dark and ordinary matter, using a two-fluid model approach. We choose the equation of state derived from the rotational curves of galaxies for dark matter and the polytropic equation of state for ordinary matter. The physical requirements for a realistic compact star are satisfied using specific parameters. For the polytropic index η=2, we find the values of observed masses, reported in our previous investigation (Mafa et al., 2020).

在本文中,我们利用双流体模型方法研究了弯曲的 Krori-Barua 时空几何,以描述由暗物质和普通物质两部分组成的紧凑恒星。对于暗物质,我们选择了从星系旋转曲线推导出的状态方程,对于普通物质,我们选择了多向性状态方程。我们使用特定的参数来满足现实中紧凑型恒星的物理要求。对于各向同性指数η=2,我们找到了先前调查(Mafa 等人,2020 年)中报告的观测质量值。
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引用次数: 0
The role of radial viscosity force and anisotropic thermal conduction in hot accretion flow 热吸积流中径向粘滞力和各向异性热传导的作用
IF 1.9 4区 物理与天体物理 Q2 ASTRONOMY & ASTROPHYSICS Pub Date : 2024-07-11 DOI: 10.1016/j.newast.2024.102276
Maryam Ghasemnezhad , Mohsen Khosravi

Recent observational evidence confirms the weak-collision dynamics of hot optically thin accretion flows around Sgr A and other nearby galactic nuclei. As a result, thermal conduction as a diffusion process can transfer the heat by electrons in a collisionless magnetized plasma. While most of the previous analytical studies consider the azimuthal viscosity, the recent studies indicated that the radial viscosity strongly affects the properties of the advection dominated accretion discs. So, in this paper, we explore the roles of two parts of anisotropic thermal conduction (parallel and perpendicular) and radial viscosity in the hot accretion disc by considering axisymmetric and steady state assumptions in the presence of outflows that can transport energy from accretion disc outward. We use the set of self-similar solutions to solve the basic equations in our present model. Our solutions reveal that transverse thermal conduction as a cooling mechanism, leads to reductions in gas temperature, disc thickness, and accretion velocity of the disc, whereas the disc rotates at a fast rate. Moreover Our solutions indicate that the perpendicular thermal conduction and the radial viscosity have opposite behavior in the physical variables of the disc. Also, our results have indicated that the anisotropic thermal conduction is significant in the parameter space of radial viscosity, outflow in the regions that the physical constraints tint,con and q,conq,con are satisfied.

最近的观测证据证实,Sgr A∗ 和其他邻近星系核周围的热光学稀薄吸积流具有弱碰撞动力学。因此,热传导作为一种扩散过程,可以通过电子在无碰撞磁化等离子体中传递热量。以往的分析研究大多考虑方位粘度,而最近的研究表明,径向粘度对平流主导吸积盘的性质影响很大。因此,在本文中,我们通过考虑轴对称和稳态假设,探讨了热吸积盘中各向异性热传导(平行和垂直)和径向粘度两部分的作用。我们使用自相似解集来求解本模型的基本方程。我们的求解结果表明,横向热传导作为一种冷却机制,会导致气体温度、圆盘厚度和圆盘的吸积速度降低,而圆盘却在快速旋转。此外,我们的求解表明,垂直热传导和径向粘度在圆盘的物理变量中具有相反的行为。同时,我们的结果还表明,在满足物理约束条件 tin≥t⊥,con 和 q∥,con⩽q⊥,con 的区域,各向异性热传导在径向粘度、外流等参数空间中具有重要作用。
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引用次数: 0
Spectral evolution and photo-ionization analysis of Nova Cas 2020 (V1391 Cas) Cas 2020 新星(V1391 Cas)的光谱演变和光电离分析
IF 1.9 4区 物理与天体物理 Q2 ASTRONOMY & ASTROPHYSICS Pub Date : 2024-07-06 DOI: 10.1016/j.newast.2024.102273
G.M. Hamed , H.H. Esenoglu , A.I. Galeev

We present spectroscopic observations of Nova Cas 2020 (V1391 Cas) obtained using the Russian Turkish Telescope during different stages of its 2020 outburst. We followed the spectral evolution of the nova until it entered the nebular phase. The expansion velocity of the ejecta reached 780km s1. The fluxes of the neutral [O I] lines at wavelengths 6300, 6364, and 5577 ̊A were used to calculate the electron temperature and the mass of neutral oxygen in the ejecta. We found average values Te=4890K, MOI=2.54×10−5M which are consistent with the values calculated for other novae. We modeled the nova’s ejected envelope 515 days after its discovery and found that the log elemental abundances by number relative to Hydrogen of the envelope are He = −0.7, C = −5.5, O = −2.5, N = −2.0 and Ne = −4.0.

我们介绍了利用俄罗斯土耳其望远镜在新星 Cas 2020(V1391 Cas)爆发的不同阶段对其进行的光谱观测。我们跟踪了新星的光谱演变过程,直到它进入星云阶段。喷出物的膨胀速度达到了 ∼780km s-1。我们利用波长为6300、6364和5577̊A的中性[O I]线的通量来计算喷出物中的电子温度和中性氧的质量。我们发现Te=4890K,MOI=2.54×10-5M⊙的平均值与其他新星的计算值一致。我们在发现新星515天后对其喷出包层进行了建模,发现包层中相对于氢的对数元素丰度为He=-0.7、C=-5.5、O=-2.5、N=-2.0和Ne=-4.0。
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New Astronomy
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