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Exploration of bulk viscous Bianchi type cosmological model in f(T) theory of gravity f(T)引力理论中的体粘性比安奇型宇宙学模型探索
IF 1.9 4区 物理与天体物理 Q2 ASTRONOMY & ASTROPHYSICS Pub Date : 2024-09-05 DOI: 10.1016/j.newast.2024.102300
P.R. Agrawal, A.P. Nile

In the present paper, the expansion of Locally Rotational Symmetric (LRS) Bianchi type - I cosmological model have been investigated with Bulk Viscous matter in the context of f(T) theory of gravity, where T signifies the torsion scalar. The power model, exponential model and linear functional model of the universe have been discussed for choices of f(T)with utilization of the special form of time dependent varying deceleration parameter. The discussion involves the examination of the dynamical behaviour of these models using some dynamical parameters and its graphical representation.

本文在 f(T) 引力理论(T 表示扭转标量)的背景下,研究了局部旋转对称(LRS)比安奇 I 型宇宙学模型与块状粘性物质的膨胀。利用随时间变化的减速参数的特殊形式,讨论了宇宙的幂模型、指数模型和线性函数模型。讨论中使用了一些动态参数及其图形表示来检验这些模型的动态行为。
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引用次数: 0
Identifying a point-symmetric morphology in supernova remnant Cassiopeia A: Explosion by jittering jets 确定仙后座A号超新星残余中的点对称形态:抖动喷流爆炸
IF 1.9 4区 物理与天体物理 Q2 ASTRONOMY & ASTROPHYSICS Pub Date : 2024-09-05 DOI: 10.1016/j.newast.2024.102307
Ealeal Bear, Noam Soker

We identify a point-symmetric morphology of the supernova remnant (SNR) Cassiopeia A compatible with shaping by at least two, and more likely more than four, pairs of opposite jets, as expected in the jittering jets explosion mechanism (JJEM) of core-collapse supernovae. Using an old Spitzer Telescope infrared map of argon, we identify seven pairs of opposite morphological features that we connect with lines that cross each other at the same point on the plane of the sky. The opposite morphological features include protrusions, clumps, filaments, and funnels in the main SNR shell. In addition to these seven symmetry axes, we find two tentative symmetry axes (lines). These lines form a point-symmetric wind-rose. We place this point-symmetric wind-rose on a new JWST and X-ray images of Cassiopeia A. We find other morphological features and one more symmetry axis that strengthen the identified point-symmetric morphology. Not all symmetry axes correspond to jets; e.g., some clumps are formed by the compression of ejecta between two jet-inflated lobes (bubbles). The robust point-symmetric morphology in the iconic Cassiopeia A SNR strongly supports the JJEM and poses a severe challenge to the neutrino-driven explosion mechanism.

我们发现仙后座A超新星残骸(SNR)的点对称形态与至少两对,更有可能是四对以上的相反喷流形成的形状相吻合,正如核心坍缩超新星的抖动喷流爆炸机制(JJEM)所预期的那样。利用旧的斯皮策望远镜氩红外图,我们确定了七对相反的形态特征,并用在天空平面上同一点相互交叉的线将它们连接起来。这些相反的形态特征包括 SNR 主外壳中的突起、团块、细丝和漏斗。除了这七条对称轴之外,我们还发现了两条暂定对称轴(线)。这些线构成了一个点对称风玫瑰图。我们将这个点对称风玫瑰放置在新的 JWST 和仙后座 A 的 X 射线图像上。我们还发现了其他形态特征和另一条对称轴,它们加强了已确定的点对称形态。并非所有的对称轴都与喷流相对应;例如,有些团块是由两个喷流充气叶片(气泡)之间的喷出物压缩形成的。标志性的仙后座A SNR中强大的点对称形态有力地支持了JJEM,并对中微子驱动的爆炸机制提出了严峻的挑战。
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引用次数: 0
A study of an X-ray flare on the solar analogue V895 Tau 太阳类似物 V895 Tau 上的 X 射线耀斑研究
IF 1.9 4区 物理与天体物理 Q2 ASTRONOMY & ASTROPHYSICS Pub Date : 2024-09-02 DOI: 10.1016/j.newast.2024.102295
Gurpreet Singh , J.C. Pandey , Umesh Yadava

Using observations with XMM-Newton, we study the characteristics of a flare emanating from a solar analogous V895 Tau. At the peak of the flare, its luminosity reached 3.3×1030 ergs1, which is 600 times more energetic than the X10 class flare on the Sun. The quiescent state corona of V895 Tau is depicted by a two-temperature plasma model with temperatures of 3.9 and 11 MK. The flare’s evolution was carefully scrutinized through time-resolved X-ray spectroscopy, unveiling the variations in temperature, emission measure, abundance and luminosity during the flare. The temperature peaked at 36.1 MK, which is approximately four times higher than the pre-flare temperature. Employing a hydrodynamic loop model, we have estimated the half length of the flaring loop to be 5.9×1010 cm. Using the loop scaling laws, other loop parameters like density, pressure, volume, and minimum magnetic field are also estimated, and are found to be similar to those of other flares from similar type of stars.

利用XMM-牛顿望远镜的观测,我们研究了太阳类似物V895 Tau发出的耀斑的特征。在耀斑的峰值,其光度达到3.3×1030 ergs-1,是太阳X10级耀斑能量的600倍。V895 Tau的静态日冕由一个温度分别为3.9和11 MK的双温等离子体模型描绘。通过时间分辨 X 射线光谱仔细观察了耀斑的演化过程,揭示了耀斑期间温度、发射尺度、丰度和光度的变化。温度峰值为 36.1 MK,大约是耀斑前温度的四倍。利用流体力学环路模型,我们估计耀斑环路的半长为 5.9×1010 厘米。利用环路缩放定律,我们还估算了其他环路参数,如密度、压力、体积和最小磁场,结果发现这些参数与来自同类恒星的其他耀斑的参数相似。
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引用次数: 0
A temperature scale of 1∼2 eV in the mass–radius relationship of white dwarfs of type DA DA 型白矮星质量-半径关系中的 1∼2 eV 温标
IF 1.9 4区 物理与天体物理 Q2 ASTRONOMY & ASTROPHYSICS Pub Date : 2024-09-02 DOI: 10.1016/j.newast.2024.102299
Jin Lim, Ji-Yu Kim, Maurice H.P.M. van Putten

The mass–radius relationship of white dwarfs (WDs) is one of their defining characteristics, largely derived from electron degeneracy pressure. We present a model-independent study of the observed mass–radius relationship in WD binaries of Parsons et al. (2017), listing data over a broad temperature range up to about 60,000 K (5 eV). The data show an appreciable temperature sensitivity with pronounced intrinsic scatter (beyond measurement uncertainty) for the canonical He-models with protontoneutron ratio 1:1. We characterize temperature sensitivity by a temperature scale T0 in model-agnostic power-law relations with temperature normalized radius. For low-mass WDs, the results identify a remarkably modest T0=12  eV. We comment on a potential interpretation for atmospheres insulating super-Eddington temperature cores from the sub-Eddington photospheres of low-mass WDs.

白矮星(WD)的质量-半径关系是其决定性特征之一,主要来自电子变性压力。我们对 Parsons 等人(2017 年)观测到的 WD 双星质量-半径关系进行了独立于模型的研究,列出了高达约 60,000 K(5 eV)的宽温度范围内的数据。对于质子-中子比为 1:1 的经典氦模型,数据显示出明显的温度灵敏度和内在散射(超出测量不确定性)。我们通过与模型无关的幂律关系中的温度标度 T0 和温度归一化半径来描述温度敏感性。对于低质量 WD,结果发现 T0=1∼2 eV 非常适中。我们对低质量WD的亚爱丁顿光球与超爱丁顿温度核心绝缘的大气层的潜在解释进行了评论。
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引用次数: 0
Inhibited destruction of dust by supernova in a clumpy medium 团块介质中超新星对尘埃的抑制性破坏
IF 1.9 4区 物理与天体物理 Q2 ASTRONOMY & ASTROPHYSICS Pub Date : 2024-09-01 DOI: 10.1016/j.newast.2024.102293
Svyatoslav Yu. Dedikov, Evgenii O. Vasiliev

The decrease rate of dust mass due to strong shock waves (vs150 km s−1) from supernovae (SNe) estimated for the Milky Way interstellar medium significantly exceeds the overall production rate by both asymptotic giant branch stars and core collapse SNe. The interplay between the production and destruction rates is critically important for evaluation of the net dust outcome from SNe at different conditions. In light of this, we study the dynamics of initially polydisperse dust grains pre-existing in an ambient medium swept up the SN shock front depending on magnitude of inhomogeneity (clumpiness) in the medium. We find that dust destruction inside the bubble is inhibited in more inhomogeneous medium: the larger amount of dust survives for the higher dispersion of density. This trend is set by the interrelation between radiative gas cooling and dust sputtering in different environment. After several radiative times the mass fraction of the survived dust saturates at the level almost independent on the gas mean density. We note that for more clumpy medium the distributions of dust over thermal phases of a gas inside the bubble and over sizes are smoother and flatter in comparison with those in a nearly homogeneous medium.

据估计,银河系星际介质中超新星(SNe)产生的强冲击波(vs≥150 km s-1)导致的尘埃质量减少率大大超过了渐近巨枝星和核心塌缩超新星的总体产生率。产生率和破坏率之间的相互作用对于评估不同条件下超新星产生的尘埃净结果至关重要。有鉴于此,我们根据介质不均匀性(团块性)的大小,研究了在SN冲击前沿扫过的环境介质中预先存在的初始多分散尘粒的动力学。我们发现,在不均匀度较高的介质中,气泡内部的尘埃破坏会受到抑制:密度分散度越高,存活的尘埃量越大。这一趋势是由不同环境中辐射气体冷却和尘埃溅射之间的相互关系决定的。经过若干辐射时间后,存活尘埃的质量分数达到饱和,几乎与气体平均密度无关。我们注意到,与近乎均匀介质中的尘埃分布相比,在更多团块状介质中,尘埃在气泡内气体热相和大小上的分布更加平滑和扁平。
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引用次数: 0
Diagnostic approaches for interacting generalized holographic Ricci dark energy models 交互广义全息利玛窦暗能量模型的诊断方法
IF 1.9 4区 物理与天体物理 Q2 ASTRONOMY & ASTROPHYSICS Pub Date : 2024-08-29 DOI: 10.1016/j.newast.2024.102298
Omar Enkhili, Farida Bargach, Dalale Mhamdi, Taoufik Ouali, Ahmed Errahmani

In this paper, we present an analytical solution for the interacting generalized holographic dark energy model, assuming a linear interaction rate between dark energy and dark matter. We determine the equation of state parameter, the generalized holographic Ricci dark energy density, the matter density, and the deceleration parameter. By analyzing the behavior of these cosmological parameters, we demonstrate that our model aligns with recent observations and reproduces the late-time accelerated expansion of the Universe. To compare our model with the ΛCDM model, we use various diagnostic tools including statefinder, Om(z)-diagnostic, statefinder hierarchy, growth rate analysis, and ωH-ωH plane. We also analyze the stability of the model by examining the speed of sound. These methods show that the dynamics of the Universe remain very close to that of the standard cosmological model.

本文假设暗能量和暗物质之间的相互作用率为线性,提出了相互作用广义全息暗能量模型的解析解。我们确定了状态方程参数、广义全息里奇暗能量密度、物质密度和减速参数。通过分析这些宇宙学参数的行为,我们证明了我们的模型与最近的观测结果一致,并再现了宇宙的晚期加速膨胀。为了将我们的模型与ΛCDM模型进行比较,我们使用了各种诊断工具,包括状态探测器、Om(z)诊断、状态探测器层次、增长率分析和ωH-ωH′平面。我们还通过研究声速分析了模型的稳定性。这些方法表明,宇宙动力学仍然非常接近标准宇宙学模型。
{"title":"Diagnostic approaches for interacting generalized holographic Ricci dark energy models","authors":"Omar Enkhili,&nbsp;Farida Bargach,&nbsp;Dalale Mhamdi,&nbsp;Taoufik Ouali,&nbsp;Ahmed Errahmani","doi":"10.1016/j.newast.2024.102298","DOIUrl":"10.1016/j.newast.2024.102298","url":null,"abstract":"<div><p>In this paper, we present an analytical solution for the interacting generalized holographic dark energy model, assuming a linear interaction rate between dark energy and dark matter. We determine the equation of state parameter, the generalized holographic Ricci dark energy density, the matter density, and the deceleration parameter. By analyzing the behavior of these cosmological parameters, we demonstrate that our model aligns with recent observations and reproduces the late-time accelerated expansion of the Universe. To compare our model with the <span><math><mi>Λ</mi></math></span>CDM model, we use various diagnostic tools including statefinder, <span><math><mrow><mi>O</mi><mi>m</mi><mrow><mo>(</mo><mi>z</mi><mo>)</mo></mrow></mrow></math></span>-diagnostic, statefinder hierarchy, growth rate analysis, and <span><math><msub><mrow><mi>ω</mi></mrow><mrow><mi>H</mi></mrow></msub></math></span>-<span><math><msubsup><mrow><mi>ω</mi></mrow><mrow><mi>H</mi></mrow><mrow><mo>′</mo></mrow></msubsup></math></span> plane. We also analyze the stability of the model by examining the speed of sound. These methods show that the dynamics of the Universe remain very close to that of the standard cosmological model.</p></div>","PeriodicalId":54727,"journal":{"name":"New Astronomy","volume":"113 ","pages":"Article 102298"},"PeriodicalIF":1.9,"publicationDate":"2024-08-29","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142096219","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
Temporal variability in transmission spectra of H2-dominated exoplanets: The influence of thermal evolution and stellar irradiation on atmospheric composition 以 H2 为主的系外行星透射光谱的时间变化:热演化和恒星辐照对大气成分的影响
IF 1.9 4区 物理与天体物理 Q2 ASTRONOMY & ASTROPHYSICS Pub Date : 2024-08-21 DOI: 10.1016/j.newast.2024.102296
Viktória Kecskeméthy , Amy Louca , Yamila Miguel
<div><p>Planets and their host stars undergo evolutionary changes over time, resulting in variations in internal temperature and incoming radiation, which significantly impact the temperature structure and composition of their atmospheres. These evolving conditions give rise to distinctive features in planetary spectra that are observable only during specific stages of planetary evolution. We aim to understand how the composition of planets with H<sub>2</sub>-dominated atmospheres changes over longer timescales due to their thermal evolution. We also investigate time-dependent features in the transmission spectra. These features could provide insights in both the formation and evolution of these gaseous planets, as well as the timescales of these changes, enabling us to study the potential variability of exoplanets over time. We evolve a <span><math><mo>∼</mo></math></span>0.04 M<span><math><msub><mrow></mrow><mrow><mi>Jup</mi></mrow></msub></math></span> and <span><math><mo>∼</mo></math></span>0.45 M<span><math><msub><mrow></mrow><mrow><mi>Jup</mi></mrow></msub></math></span> planet around a 1.0 M<span><math><msub><mrow></mrow><mrow><mo>⊙</mo></mrow></msub></math></span> and 1.3 M<span><math><msub><mrow></mrow><mrow><mo>⊙</mo></mrow></msub></math></span> star respectively for 10<span><math><msup><mrow></mrow><mrow><mn>9</mn><mo>.</mo><mn>5</mn></mrow></msup></math></span> years. In both systems, the planets are considered at semi-major axes of 0.1 AU and 1.0 AU. The star-planet systems are evolved by making use of Modules for Experiments in Stellar Astrophysics (MESA). The temperature–pressure profiles are obtained at selected time-steps using an analytical approximation based on the internal and irradiation temperature of the planet at each time step. We then use VULCAN, a photochemical kinetics code, to see how the composition changes with time in the atmosphere due to the thermal evolution of the planets. By making use of the radiative transfer code petitRADTrans, we also simulate the evolution of the transmission spectra of the planets to find potential time-dependent spectral features. Our findings show a prominent change in the CO<span><math><msub><mrow></mrow><mrow><mn>2</mn></mrow></msub></math></span> feature at <span><math><mrow><mo>∼</mo><mn>4</mn><mo>.</mo><mn>3</mn><mi>μ</mi><mi>m</mi></mrow></math></span>. For the 0.45 M<span><math><msub><mrow></mrow><mrow><mi>Jup</mi></mrow></msub></math></span> case, this feature is visible in the pre-main-sequence phase of the host star, regardless of orbital distance from the host star. In the case of the <span><math><mo>∼</mo></math></span>0.04 M<span><math><msub><mrow></mrow><mrow><mi>Jup</mi></mrow></msub></math></span> planet, this CO<sub>2</sub> feature is visible until t <span><math><mo>≤</mo></math></span> 10<sup>6</sup> years, and then it reappears after t <span><math><mo>≥</mo></math></span> 10<sup>8</sup> years when the planet is 0.1 AU away the host star. The CH<sub>4</sub> features
行星及其宿主恒星会随着时间的推移而发生演化变化,导致内部温度和入射辐射的变化,从而对其大气层的温度结构和成分产生重大影响。这些不断变化的条件导致行星光谱中出现了只有在行星演化的特定阶段才能观测到的独特特征。我们的目标是了解以 H2 为主的行星大气成分如何因其热演化而在更长的时间尺度上发生变化。我们还研究了透射光谱中随时间变化的特征。这些特征可以让我们了解这些气态行星的形成和演化,以及这些变化的时间尺度,从而研究系外行星随时间的潜在变化。我们分别围绕一颗1.0 M⊙恒星和一颗1.3 M⊙恒星演化了一颗∼0.04 MJup和一颗∼0.45 MJup行星,历时109.5年。在这两个系统中,行星的半主轴分别为 0.1 AU 和 1.0 AU。恒星-行星系统是利用恒星天体物理学实验模块(MESA)演化而成的。在选定的时间步长内,根据行星在每个时间步长内的内部温度和辐照温度,使用分析近似方法获得温度-压力剖面。然后,我们使用光化学动力学代码 VULCAN 来观察由于行星的热演化,大气中的成分如何随时间发生变化。通过使用辐射传递代码 petitRADTrans,我们还模拟了行星透射光谱的演变,以发现潜在的随时间变化的光谱特征。我们的研究结果表明,在 ∼4.3μm 处的 CO2 特征发生了显著变化。在 0.45 MJup 的情况下,无论与主星的轨道距离如何,这一特征在主星的前主序阶段都是可见的。在 ∼0.04 MJup 行星的情况下,这一 CO2 特征在 t≤106 年之前是可见的,然后在 t≥108 年之后,当行星距离宿主恒星 0.1 AU 时再次出现。由于早期的高温有利于 CO2 而非 CH4,因此只有当行星距离主恒星 0.1 AU 并经历高辐照时,CH4 在 ∼3.3μm 和 ∼7.5μm 处的特征才与时间有关。当行星距离其主恒星1.0 AU时,无论行星的质量和内部温度如何,CH4特征总是可见的。
{"title":"Temporal variability in transmission spectra of H2-dominated exoplanets: The influence of thermal evolution and stellar irradiation on atmospheric composition","authors":"Viktória Kecskeméthy ,&nbsp;Amy Louca ,&nbsp;Yamila Miguel","doi":"10.1016/j.newast.2024.102296","DOIUrl":"10.1016/j.newast.2024.102296","url":null,"abstract":"&lt;div&gt;&lt;p&gt;Planets and their host stars undergo evolutionary changes over time, resulting in variations in internal temperature and incoming radiation, which significantly impact the temperature structure and composition of their atmospheres. These evolving conditions give rise to distinctive features in planetary spectra that are observable only during specific stages of planetary evolution. We aim to understand how the composition of planets with H&lt;sub&gt;2&lt;/sub&gt;-dominated atmospheres changes over longer timescales due to their thermal evolution. We also investigate time-dependent features in the transmission spectra. These features could provide insights in both the formation and evolution of these gaseous planets, as well as the timescales of these changes, enabling us to study the potential variability of exoplanets over time. We evolve a &lt;span&gt;&lt;math&gt;&lt;mo&gt;∼&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt;0.04 M&lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;Jup&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt; and &lt;span&gt;&lt;math&gt;&lt;mo&gt;∼&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt;0.45 M&lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;Jup&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt; planet around a 1.0 M&lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;⊙&lt;/mo&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt; and 1.3 M&lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;⊙&lt;/mo&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt; star respectively for 10&lt;span&gt;&lt;math&gt;&lt;msup&gt;&lt;mrow&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;9&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;5&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/math&gt;&lt;/span&gt; years. In both systems, the planets are considered at semi-major axes of 0.1 AU and 1.0 AU. The star-planet systems are evolved by making use of Modules for Experiments in Stellar Astrophysics (MESA). The temperature–pressure profiles are obtained at selected time-steps using an analytical approximation based on the internal and irradiation temperature of the planet at each time step. We then use VULCAN, a photochemical kinetics code, to see how the composition changes with time in the atmosphere due to the thermal evolution of the planets. By making use of the radiative transfer code petitRADTrans, we also simulate the evolution of the transmission spectra of the planets to find potential time-dependent spectral features. Our findings show a prominent change in the CO&lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt; feature at &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mo&gt;∼&lt;/mo&gt;&lt;mn&gt;4&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;3&lt;/mn&gt;&lt;mi&gt;μ&lt;/mi&gt;&lt;mi&gt;m&lt;/mi&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt;. For the 0.45 M&lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;Jup&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt; case, this feature is visible in the pre-main-sequence phase of the host star, regardless of orbital distance from the host star. In the case of the &lt;span&gt;&lt;math&gt;&lt;mo&gt;∼&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt;0.04 M&lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;Jup&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt; planet, this CO&lt;sub&gt;2&lt;/sub&gt; feature is visible until t &lt;span&gt;&lt;math&gt;&lt;mo&gt;≤&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt; 10&lt;sup&gt;6&lt;/sup&gt; years, and then it reappears after t &lt;span&gt;&lt;math&gt;&lt;mo&gt;≥&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt; 10&lt;sup&gt;8&lt;/sup&gt; years when the planet is 0.1 AU away the host star. The CH&lt;sub&gt;4&lt;/sub&gt; features ","PeriodicalId":54727,"journal":{"name":"New Astronomy","volume":"113 ","pages":"Article 102296"},"PeriodicalIF":1.9,"publicationDate":"2024-08-21","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S1384107624001106/pdfft?md5=d658e35eb5e86085855c30c9d7f75b81&pid=1-s2.0-S1384107624001106-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142040012","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
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。
{"title":"The size and shape dependence of the SDSS galaxy bispectrum","authors":"Anindita Nandi ,&nbsp;Sukhdeep Singh Gill ,&nbsp;Debanjan Sarkar ,&nbsp;Abinash Kumar Shaw ,&nbsp;Biswajit Pandey ,&nbsp;Somnath Bharadwaj","doi":"10.1016/j.newast.2024.102292","DOIUrl":"10.1016/j.newast.2024.102292","url":null,"abstract":"&lt;div&gt;&lt;p&gt;We have measured the spherically averaged bispectrum of the SDSS main galaxy sample, considering a volume-limited &lt;span&gt;&lt;math&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mrow&gt;&lt;mo&gt;[&lt;/mo&gt;&lt;mn&gt;296&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;75&lt;/mn&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;mi&gt;Mpc&lt;/mi&gt;&lt;mo&gt;]&lt;/mo&gt;&lt;/mrow&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;3&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/math&gt;&lt;/span&gt; data cube with mean galaxy number density &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;63&lt;/mn&gt;&lt;mo&gt;×&lt;/mo&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mn&gt;10&lt;/mn&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;3&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&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;3&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt; and median redshift &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;102&lt;/mn&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt;. 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}
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