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Pulsational and eclipsing nature of TIC 140736015 TIC 140736015 的脉动和蚀变性质
IF 1.9 4区 物理与天体物理 Q2 ASTRONOMY & ASTROPHYSICS Pub Date : 2024-06-29 DOI: 10.1016/j.newast.2024.102271
B. Gürol , A.-Y. Zhou

We present the discovery of γ Doradus-type pulsations in the eclipsing binary TIC 140736015. We obtained the physical and geometrical parameters of this detached eclipsing binary hosting a pulsating component. Based on the Transiting Exoplanet Survey Satellite (TESS) observation and Gaia DR3 data of TIC 140736015, we refined the light elements of the system using (OC) analysis and found that the eclipse times varied with a period of 2048 days, probably linked to the multiperiodic pulsational nature. We showed that essentially, only secondary eclipse is seen in the phased light curve. The frequency analysis using the out-of-eclipse data reveals that all the pulsational frequencies are located in the region lower than 5d1. After removing the pulsational variation from the observations we analysed the residual light curve together with the radial velocity data obtained from Gaia DR3 and find the masses and radii of the primary and secondary components as M1=1.429±0.022 M, M2=1.402±0.022 Mand R1=1.685±0.001 R, R2=1.393±0.001 R, respectively. Regarding the location of the components on the Hertzsprung–Russell diagram both components can be a γ Dor/solar-like pulsator.

我们在食双星 TIC 140736015 中发现了多拉杜斯型脉冲。我们获得了这个包含脉冲成分的分离食双星的物理和几何参数。根据TIC 140736015的凌日系外行星巡天卫星()观测数据和盖亚DR3数据,我们通过分析完善了该系统的光元素,并发现日食时间以天为周期变化,这可能与多周期脉冲性质有关。我们发现,在相位光曲线中基本上只能看到次食。利用日食外数据进行的频率分析表明,所有脉冲频率都位于低于......的区域。 从观测数据中剔除脉冲变化后,我们将残余光曲线与从盖亚 DR3 获得的径向速度数据一起进行了分析,发现主成分和副成分的质量和半径分别为......和......。从这两个成分在赫兹普朗-拉塞尔图上的位置来看,它们都可能是类似于多/太阳的脉动器。
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引用次数: 0
First photometric study of W UMa-type binary systems: BK Vul and V699 Cep 对 W UMa 型双星系统的首次光度研究:BK Vul 和 V699 Cep
IF 1.9 4区 物理与天体物理 Q2 ASTRONOMY & ASTROPHYSICS Pub Date : 2024-06-29 DOI: 10.1016/j.newast.2024.102270
S. Adalalı , E. Soydugan

In this study, new CCD photometric observations and photometric analysis of BK Vul and V699 Cep systems, which are classified as contact binaries in the literature, are presented. For the V699 Cep, the TESS light curve was also used in the photometric analysis. We determined the basic astrophysical parameters of the BK Vul and V699 Cep systems from photometric analysis using the Wilson–Devinney method. Due to the lack of spectroscopic data for both systems in the literature, these absolute parameters were approximately calculated as to be M2 = 0.73 M, R1 = 1.39 R and R2 = 1.09 R for BK Vul, and M2 = 0.36 M, R1 = 2.40 R and R2 = 1.33 R for V699 Cep after estimating the mass of the primary component. The period decrease rate (dP/dt) and cyclic variation period of BK Vul were determined from the OC analysis as -3.86 ×107 day yr−1 and 27 yrs., respectively. The evolutionary status of components of both systems were discussed.

本研究介绍了对 BK Vul 和 V699 Cep 系统的新 CCD 测光观测结果和测光分析,这两个系统在文献中被归类为接触双星。对于 V699 Cep,TESS 光曲线也被用于光度分析。我们利用威尔逊-德文尼(Wilson-Devinney)方法通过测光分析确定了BK Vul和V699 Cep系统的基本天体物理参数。由于文献中缺乏这两个系统的光谱数据,在估算出主成分的质量后,这些绝对参数被近似计算为:BK Vul 的绝对参数为 M2 = 0.73 M⊙,R1 = 1.39 R⊙,R2 = 1.09 R⊙;V699 Cep 的绝对参数为 M2 = 0.36 M⊙,R1 = 2.40 R⊙,R2 = 1.33 R⊙。通过O-C分析确定BK Vul的周期下降率(dP/dt)和周期变化周期分别为-3.86×10-7天/年和27年。讨论了这两个系统各组成部分的演化状况。
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引用次数: 0
First light simultaneous triple-channel optical observations of the OPTICAM system at the OAN-SPM 在 OAN-SPM 对 OPTICAM 系统进行首次三通道同步光学观测
IF 1.9 4区 物理与天体物理 Q2 ASTRONOMY & ASTROPHYSICS Pub Date : 2024-06-25 DOI: 10.1016/j.newast.2024.102262
Angel Castro , Raúl Michel , Noel Castro Segura , Diego Altamirano , Carlos Tejada , Joel Herrera , Enrique Colorado , Gerardo Sierra , Liliana Altamirano-Dévora , Juan Echevarría , Rasjied Sloot , Rudy Wijnands , Iván Zavala , David Rojas , Juan V. Hernández Santisteban , Federico Vincentelli , Javier A. Hernández-Landa , Song Wang , Melissa Fuentes , Poshak Gandhi , Francisco Valenzuela

OPTICAM is a triple-band optical system developed for the 2.1 m telescope of the National Astronomical Observatory in the Sierra de San Pedro Mártir (OAN-SPM). Partial engineering tests were conducted in 2019, with the complete system experiencing its first light in March 2022. The system incorporates two beam splitters, enabling simultaneous observations on three channels. Users can choose three out of the five available filters from the SDSS filter set (ugriz), covering the wavelength range from 320 to 1000 nm. It offers an effective field of view of approximately 4.7, 4.7, and 5.6 arcminutes in each of its arms, respectively. Due to its design and capabilities, OPTICAM is suitable for coordinated observations with other ground-based and space-based observatories. This document presents the final instrument design and the current system status. Some of the optical tests carried out are described. We also present the results of scientific observations conducted during its first light and first year of operations.

OPTICAM 是为圣佩德罗马蒂尔山脉国家天文台(OAN-SPM)的 2.1 米望远镜开发的三波段光学系统。2019 年进行了部分工程测试,整个系统将于 2022 年 3 月首次点亮。该系统包含两个分光镜,可在三个频道上同时进行观测。用户可以从 SDSS 滤光片组()的五个可用滤光片中选择三个,波长范围从 320 纳米到 1000 纳米。它的每个臂的有效视场分别约为 4.7、4.7 和 5.6 弧分。由于其设计和功能,OPTICAM 适合与其他地面和空间观测站进行协调观测。本文件介绍了仪器的最终设计和目前的系统状况。介绍了已进行的一些光学测试。我们还介绍了在其首次点亮和第一年运行期间进行的科学观测的结果。
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引用次数: 0
Measurable parameter combinations of environmentally-dephased EMRI gravitational-wave signals 环境相减 EMRI 重力波信号的可测量参数组合
IF 2 4区 物理与天体物理 Q2 ASTRONOMY & ASTROPHYSICS Pub Date : 2024-06-08 DOI: 10.1016/j.newast.2024.102263
Marco Immanuel B. Rivera , Reinabelle C. Reyes

The future space-borne Laser Interferometer Space Antenna (LISA) is expected to detect gravitational waves (GW) from Extreme Mass Ratio Inspiral (EMRI) binaries which may live in nontrivial environments such as accretion disks. In this work, we apply the Fisher matrix Principal Component Analysis (PCA) method to assess how well LISA observations can jointly constrain the source parameters and environmental densities around EMRIs. Specifically, we calculate the Fisher matrix from the post-Newtonian parameters of an EMRI binary embedded in a fluid with a constant density profile. We determine that the most dominant measurable parameter combination is dominated by contributions from environmental effects, namely, gravitational drag, accretion, and gravitational pull (in order of contribution). The proposed reparameterization of the PN parameters can be used to improve the power and efficiency of future detection and parameter estimation methods.

未来的星载激光干涉仪空间天线(LISA)有望探测到来自极端质量比激发(EMRI)双星的引力波(GW),这些双星可能生活在吸积盘等非简单环境中。在这项工作中,我们应用费舍尔矩阵主成分分析(PCA)方法来评估 LISA 观测能在多大程度上共同约束 EMRI 周围的源参数和环境密度。具体来说,我们根据嵌入恒定密度曲线流体中的 EMRI 双星的后牛顿参数计算费雪矩阵。我们确定,最主要的可测量参数组合是由环境效应贡献的,即引力拖拽、吸积和引力(按贡献大小排序)。提议的 PN 参数重新参数化可以用来提高未来探测和参数估计方法的功率和效率。
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引用次数: 0
OSIRIS-GR: General relativistic activation of the polar cap of a compact neutron star OSIRIS-GR:紧凑型中子星极盖的广义相对论激活
IF 2 4区 物理与天体物理 Q2 ASTRONOMY & ASTROPHYSICS Pub Date : 2024-06-04 DOI: 10.1016/j.newast.2024.102261
R. Torres , T. Grismayer , F. Cruz , R.A. Fonseca , L.O. Silva

We present ab initio global general-relativistic Particle-in-cell (GR-PIC) simulations of compact millisecond neutron star magnetospheres in the axisymmetric aligned rotator configuration. We investigate the role of GR and plasma supply on the polar cap particle acceleration efficiency – the precursor of coherent radio emission – employing a new module for the PIC code OSIRIS, designed to model plasma dynamics around compact objects with fully self-consistent GR effects. We provide a detailed description of the main sub-algorithms of the novel PIC algorithm, including a charge-conserving current deposit scheme for curvilinear coordinates. We demonstrate efficient particle acceleration in the polar caps of compact neutron stars with denser magnetospheres, numerically validating the spacelike current extension provided by force-free models. We show that GR relaxes the minimum required poloidal magnetospheric current for the transition of the polar cap to the accelerator regime, thus justifying the observation of weak pulsars beyond the expected death line. We denote that spin-down luminosity intermittency and radio pulse nullings for older pulsars might arise from the interplay between the polar and outer gaps. Also, narrower radio beams are expected for weaker low-obliquity pulsars.

我们介绍了对轴对称对齐转子构型的紧凑型毫秒中子星磁层进行的全局广义相对论粒子入胞(GR-PIC)模拟。我们利用 PIC 代码 OSIRIS 的一个新模块研究了 GR 和等离子体供应对极盖粒子加速效率(相干射电发射的前兆)的作用,该模块旨在利用完全自洽的 GR 效应模拟紧凑天体周围的等离子体动力学。我们详细介绍了新型 PIC 算法的主要子算法,包括曲线坐标的电荷守恒电流沉积方案。我们证明了粒子在具有较密集磁层的紧凑中子星极盖中的高效加速,从数值上验证了无力模型所提供的类似于空间的电流扩展。我们表明,GR 放松了极盖过渡到加速器机制所需的最小极磁层电流,从而证明了在预期死亡线之外观测到弱脉冲星是合理的。我们指出,较老脉冲星的自旋下降光度间歇和射电脉冲无效可能是由于极隙和外隙之间的相互作用造成的。另外,较弱的低倾脉冲星的射电波束预计会更窄。
{"title":"OSIRIS-GR: General relativistic activation of the polar cap of a compact neutron star","authors":"R. Torres ,&nbsp;T. Grismayer ,&nbsp;F. Cruz ,&nbsp;R.A. Fonseca ,&nbsp;L.O. Silva","doi":"10.1016/j.newast.2024.102261","DOIUrl":"https://doi.org/10.1016/j.newast.2024.102261","url":null,"abstract":"<div><p>We present ab initio global general-relativistic Particle-in-cell (GR-PIC) simulations of compact millisecond neutron star magnetospheres in the axisymmetric aligned rotator configuration. We investigate the role of GR and plasma supply on the polar cap particle acceleration efficiency – the precursor of coherent radio emission – employing a new module for the PIC code OSIRIS, designed to model plasma dynamics around compact objects with fully self-consistent GR effects. We provide a detailed description of the main sub-algorithms of the novel PIC algorithm, including a charge-conserving current deposit scheme for curvilinear coordinates. We demonstrate efficient particle acceleration in the polar caps of compact neutron stars with denser magnetospheres, numerically validating the spacelike current extension provided by force-free models. We show that GR relaxes the minimum required poloidal magnetospheric current for the transition of the polar cap to the accelerator regime, thus justifying the observation of weak pulsars beyond the expected death line. We denote that spin-down luminosity intermittency and radio pulse nullings for older pulsars might arise from the interplay between the polar and outer gaps. Also, narrower radio beams are expected for weaker low-obliquity pulsars.</p></div>","PeriodicalId":54727,"journal":{"name":"New Astronomy","volume":"112 ","pages":"Article 102261"},"PeriodicalIF":2.0,"publicationDate":"2024-06-04","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S1384107624000757/pdfft?md5=4b7e74c6e0596423df64b16f4a75d011&pid=1-s2.0-S1384107624000757-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141291525","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
Kinematical and ellipsoidal properties of the inner-halo hot subdwarfs observed in Gaia DR3 and LAMOST DR7 盖亚DR3和LAMOST DR7观测到的内光环热亚矮星的运动学和椭球特性
IF 2 4区 物理与天体物理 Q2 ASTRONOMY & ASTROPHYSICS Pub Date : 2024-06-03 DOI: 10.1016/j.newast.2024.102258
W.H. Elsanhoury
<div><p>Here, we report the kinematical parameters of inner-halo hot subdwarfs located within <span><math><mrow><mo>(</mo><mrow><mi>d</mi><mo>≤</mo><mn>15</mn><mrow><mspace></mspace><mtext>kpc</mtext></mrow></mrow><mo>)</mo></mrow></math></span> at high Galactic latitudes <span><math><mrow><mo>(</mo><mrow><msup><mrow><mi>b</mi></mrow><mi>o</mi></msup><mo>≥</mo><mn>20</mn></mrow><mo>)</mo></mrow></math></span>. The study included three program stars for one of the extreme He-rich groups (<em>e</em>He-1) with eccentricity (<em>e</em>= 0.65) and the z-component of the angular momentum (J<sub>z</sub> = 4288.66 kpc km <em>s</em><sup>−1</sup>), the inner halo program I with 121 points <span><math><mrow><mo>(</mo><mrow><msub><mi>T</mi><mtext>eff</mtext></msub><mo>≥</mo><mn>24</mn><mo>,</mo><mn>000</mn></mrow><mo>)</mo></mrow></math></span> and their subsections, i.e. inner halo program II (sdB; 79 points) with <span><math><mrow><mo>(</mo><mrow><mn>40</mn><mo>,</mo><mn>000</mn><mo>≥</mo><msub><mi>T</mi><mtext>eff</mtext></msub><mo>≥</mo><mn>24</mn><mo>,</mo><mn>000</mn></mrow><mo>)</mo></mrow></math></span> and inner halo program III (sdO; 42 points) with <span><math><mrow><mo>(</mo><mrow><mn>80</mn><mo>,</mo><mn>000</mn><mo>≥</mo><msub><mi>T</mi><mtext>eff</mtext></msub><mo>≥</mo><mn>40</mn><mo>,</mo><mn>000</mn></mrow><mo>)</mo></mrow></math></span>. First, we calculated the spatial velocities (<span><math><mrow><mover><mi>U</mi><mo>¯</mo></mover><mo>,</mo><mrow><mspace></mspace><mover><mi>V</mi><mo>¯</mo></mover></mrow><mo>,</mo><mrow><mspace></mspace><mover><mi>W</mi><mo>¯</mo></mover></mrow><mo>;</mo><mrow><mspace></mspace><mtext>km</mtext><mspace></mspace></mrow><msup><mrow><mi>s</mi></mrow><mrow><mo>−</mo><mn>1</mn></mrow></msup><mrow><mo>)</mo></mrow></mrow></math></span> along the Galactic coordinates (i.e., 25.73 ± ± 5.07, 28.79 ± 5.37, −14.51 ± 3.81) and their dispersion velocities <span><math><mrow><mo>(</mo><mrow><msub><mi>σ</mi><mn>1</mn></msub><mo>,</mo><mspace></mspace><msub><mi>σ</mi><mn>2</mn></msub><mo>,</mo><mspace></mspace><msub><mi>σ</mi><mn>3</mn></msub><mo>;</mo><mrow><mspace></mspace><mtext>km</mtext><mspace></mspace></mrow><msup><mrow><mi>s</mi></mrow><mrow><mo>−</mo><mn>1</mn></mrow></msup></mrow><mo>)</mo></mrow></math></span> = (161.94 ± 12.73, 140.31 ± 11.85, 101.57 ± 10.08) and subsequently their subsections sdB and sdO. Second, we calculated the vertex longitudes <span><math><mrow><mo>(</mo><msub><mi>l</mi><mn>2</mn></msub><mo>)</mo></mrow></math></span> and the Solar motion <span><math><mrow><mo>(</mo><mrow><msub><mi>S</mi><mo>⊙</mo></msub><mo>=</mo><mn>41.24</mn><mrow><mspace></mspace><mspace></mspace></mrow><mn>6.42</mn><mrow><mspace></mspace><mtext>km</mtext><mspace></mspace></mrow><msup><mrow><mi>s</mi></mrow><mrow><mo>−</mo><mn>1</mn></mrow></msup></mrow><mo>)</mo></mrow></math></span> as well as their subsections. Finally, based on the kinematic relation of the ratio <span><math><mrow><mo>(</mo><mrow><msub><mi>σ</mi
在这里,我们报告了位于银河系高纬度(bo≥20)(d≤15kpc)范围内的内光环热亚矮星的运动学参数。该研究包括三颗程序恒星,它们属于极端富氦群组(eHe-1)之一,其偏心率(e= 0.65)和角动量的 z 分量(Jz = 4288.66 kpc km s-1)的内光环计划 I,包括 121 个点(Teff≥24,000)及其子部分,即内光环计划 II(sdB;79 个点)(40,000≥Teff≥24,000)和内光环计划 III(sdO;42 个点)(80,000≥Teff≥40,000)。首先,我们计算了沿银河系坐标(即 25.73 ± ± 5.07, 28.79 ± 5.37, -14.51 ± 3.81)的空间速度(U¯,V¯,W¯;kms-1)和它们的色散速度(σ1,σ2,σ3;kms-1)= (161.94 ± 12.73, 140.31 ± 11.85, 101.57 ± 10.08),随后又计算了它们的分段 sdB 和 sdO。其次,我们计算了顶点经度(l2)和太阳运动(S⊙=41.246.42kms-1)及其分段。最后,根据比率(σ2/σ1)的运动学关系和我们之前计算的角旋转率数值(|A-B|=26.07±5.10;kms-1kpc-1),我们得到了平均奥尔特常数为 (A&B;kms-1kpc-1) = (9.38 ± 0.33, -16.69±0.25)。
{"title":"Kinematical and ellipsoidal properties of the inner-halo hot subdwarfs observed in Gaia DR3 and LAMOST DR7","authors":"W.H. Elsanhoury","doi":"10.1016/j.newast.2024.102258","DOIUrl":"https://doi.org/10.1016/j.newast.2024.102258","url":null,"abstract":"&lt;div&gt;&lt;p&gt;Here, we report the kinematical parameters of inner-halo hot subdwarfs located within &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mrow&gt;&lt;mi&gt;d&lt;/mi&gt;&lt;mo&gt;≤&lt;/mo&gt;&lt;mn&gt;15&lt;/mn&gt;&lt;mrow&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;mtext&gt;kpc&lt;/mtext&gt;&lt;/mrow&gt;&lt;/mrow&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt; at high Galactic latitudes &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mrow&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;b&lt;/mi&gt;&lt;/mrow&gt;&lt;mi&gt;o&lt;/mi&gt;&lt;/msup&gt;&lt;mo&gt;≥&lt;/mo&gt;&lt;mn&gt;20&lt;/mn&gt;&lt;/mrow&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt;. The study included three program stars for one of the extreme He-rich groups (&lt;em&gt;e&lt;/em&gt;He-1) with eccentricity (&lt;em&gt;e&lt;/em&gt;= 0.65) and the z-component of the angular momentum (J&lt;sub&gt;z&lt;/sub&gt; = 4288.66 kpc km &lt;em&gt;s&lt;/em&gt;&lt;sup&gt;−1&lt;/sup&gt;), the inner halo program I with 121 points &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mrow&gt;&lt;msub&gt;&lt;mi&gt;T&lt;/mi&gt;&lt;mtext&gt;eff&lt;/mtext&gt;&lt;/msub&gt;&lt;mo&gt;≥&lt;/mo&gt;&lt;mn&gt;24&lt;/mn&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mn&gt;000&lt;/mn&gt;&lt;/mrow&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt; and their subsections, i.e. inner halo program II (sdB; 79 points) with &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mrow&gt;&lt;mn&gt;40&lt;/mn&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mn&gt;000&lt;/mn&gt;&lt;mo&gt;≥&lt;/mo&gt;&lt;msub&gt;&lt;mi&gt;T&lt;/mi&gt;&lt;mtext&gt;eff&lt;/mtext&gt;&lt;/msub&gt;&lt;mo&gt;≥&lt;/mo&gt;&lt;mn&gt;24&lt;/mn&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mn&gt;000&lt;/mn&gt;&lt;/mrow&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt; and inner halo program III (sdO; 42 points) with &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mrow&gt;&lt;mn&gt;80&lt;/mn&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mn&gt;000&lt;/mn&gt;&lt;mo&gt;≥&lt;/mo&gt;&lt;msub&gt;&lt;mi&gt;T&lt;/mi&gt;&lt;mtext&gt;eff&lt;/mtext&gt;&lt;/msub&gt;&lt;mo&gt;≥&lt;/mo&gt;&lt;mn&gt;40&lt;/mn&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mn&gt;000&lt;/mn&gt;&lt;/mrow&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt;. First, we calculated the spatial velocities (&lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mover&gt;&lt;mi&gt;U&lt;/mi&gt;&lt;mo&gt;¯&lt;/mo&gt;&lt;/mover&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mrow&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;mover&gt;&lt;mi&gt;V&lt;/mi&gt;&lt;mo&gt;¯&lt;/mo&gt;&lt;/mover&gt;&lt;/mrow&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mrow&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;mover&gt;&lt;mi&gt;W&lt;/mi&gt;&lt;mo&gt;¯&lt;/mo&gt;&lt;/mover&gt;&lt;/mrow&gt;&lt;mo&gt;;&lt;/mo&gt;&lt;mrow&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;mtext&gt;km&lt;/mtext&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;/mrow&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;s&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;/math&gt;&lt;/span&gt; along the Galactic coordinates (i.e., 25.73 ± ± 5.07, 28.79 ± 5.37, −14.51 ± 3.81) and their dispersion velocities &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mrow&gt;&lt;msub&gt;&lt;mi&gt;σ&lt;/mi&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/msub&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;msub&gt;&lt;mi&gt;σ&lt;/mi&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/msub&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;msub&gt;&lt;mi&gt;σ&lt;/mi&gt;&lt;mn&gt;3&lt;/mn&gt;&lt;/msub&gt;&lt;mo&gt;;&lt;/mo&gt;&lt;mrow&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;mtext&gt;km&lt;/mtext&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;/mrow&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;s&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;/math&gt;&lt;/span&gt; = (161.94 ± 12.73, 140.31 ± 11.85, 101.57 ± 10.08) and subsequently their subsections sdB and sdO. Second, we calculated the vertex longitudes &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;msub&gt;&lt;mi&gt;l&lt;/mi&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/msub&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt; and the Solar motion &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mrow&gt;&lt;msub&gt;&lt;mi&gt;S&lt;/mi&gt;&lt;mo&gt;⊙&lt;/mo&gt;&lt;/msub&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mn&gt;41.24&lt;/mn&gt;&lt;mrow&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;/mrow&gt;&lt;mn&gt;6.42&lt;/mn&gt;&lt;mrow&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;mtext&gt;km&lt;/mtext&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;/mrow&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;s&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;/math&gt;&lt;/span&gt; as well as their subsections. Finally, based on the kinematic relation of the ratio &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mrow&gt;&lt;msub&gt;&lt;mi&gt;σ&lt;/mi","PeriodicalId":54727,"journal":{"name":"New Astronomy","volume":"112 ","pages":"Article 102258"},"PeriodicalIF":2.0,"publicationDate":"2024-06-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141291524","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
Observational constraints on modified CPL models considering non-cold dark matter 考虑非冷暗物质的修正 CPL 模型的观测约束
IF 2 4区 物理与天体物理 Q2 ASTRONOMY & ASTROPHYSICS Pub Date : 2024-06-01 DOI: 10.1016/j.newast.2024.102259
Gopal Sardar, Subenoy Chakraborty

In the present work we consider three modified Chevallier–Polarski–Linder (CPL) models with considering non-cold dark matter in the background of homogeneous and isotropic FLRW space–time model. From the observational data set ((Pantheon+)+BAO+HST) we find that all the parameters involved in the models having equation of dark energy state ωde=ω0+ω1a(1+a)p (Model II) and ωde=ω0+ω11a(1+a)p (Model III) do not depend on p. We also find that for all the models equation of state for dark matter is almost same and observe that Model I is more preferable than the other two proposed models.

在本研究中,我们考虑了三个修正的切瓦利埃-波兰斯基-林德(CPL)模型,其中考虑了在均质和各向同性的 FLRW 时空模型背景下的非冷暗物质。从观测数据集((Pantheon+)+BAO+HST)中我们发现,暗能量状态方程为ωde=ω0+ω1a(1+a)p(模型II)和ωde=ω0+ω11-a(1+a)p(模型III)的模型所涉及的所有参数都不依赖于p。
{"title":"Observational constraints on modified CPL models considering non-cold dark matter","authors":"Gopal Sardar,&nbsp;Subenoy Chakraborty","doi":"10.1016/j.newast.2024.102259","DOIUrl":"10.1016/j.newast.2024.102259","url":null,"abstract":"<div><p>In the present work we consider three modified Chevallier–Polarski–Linder (CPL) models with considering non-cold dark matter in the background of homogeneous and isotropic FLRW space–time model. From the observational data set ((Pantheon+)+BAO+HST) we find that all the parameters involved in the models having equation of dark energy state <span><math><mrow><msub><mrow><mi>ω</mi></mrow><mrow><mi>d</mi><mi>e</mi></mrow></msub><mo>=</mo><msub><mrow><mi>ω</mi></mrow><mrow><mn>0</mn></mrow></msub><mo>+</mo><msub><mrow><mi>ω</mi></mrow><mrow><mn>1</mn></mrow></msub><mfrac><mrow><mi>a</mi></mrow><mrow><msup><mrow><mrow><mo>(</mo><mn>1</mn><mo>+</mo><mi>a</mi><mo>)</mo></mrow></mrow><mrow><mi>p</mi></mrow></msup></mrow></mfrac></mrow></math></span> (Model II) and <span><math><mrow><msub><mrow><mi>ω</mi></mrow><mrow><mi>d</mi><mi>e</mi></mrow></msub><mo>=</mo><msub><mrow><mi>ω</mi></mrow><mrow><mn>0</mn></mrow></msub><mo>+</mo><msub><mrow><mi>ω</mi></mrow><mrow><mn>1</mn></mrow></msub><mfrac><mrow><mn>1</mn><mo>−</mo><mi>a</mi></mrow><mrow><msup><mrow><mrow><mo>(</mo><mn>1</mn><mo>+</mo><mi>a</mi><mo>)</mo></mrow></mrow><mrow><mi>p</mi></mrow></msup></mrow></mfrac></mrow></math></span> (Model III) do not depend on <span><math><mi>p</mi></math></span>. We also find that for all the models equation of state for dark matter is almost same and observe that Model I is more preferable than the other two proposed models.</p></div>","PeriodicalId":54727,"journal":{"name":"New Astronomy","volume":"112 ","pages":"Article 102259"},"PeriodicalIF":2.0,"publicationDate":"2024-06-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141277508","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
Spectroscopic and photometric investigations of the totally eclipsing contact binary V1320 Cas 全食接触双星 V1320 Cas 的光谱和光度研究
IF 2 4区 物理与天体物理 Q2 ASTRONOMY & ASTROPHYSICS Pub Date : 2024-05-31 DOI: 10.1016/j.newast.2024.102254
Jian-Fei Liu , Kai Li , Xu Chen , Ke-Xin Li , Fei Liu , Xing Gao , Guo-You Sun

We analyzed the light curve of the total eclipse contact binary V1320 Cas, obtained reliable photometric solutions, confirmed it to be a W-type contact binary with a mass ratio of 3.404 and a contact degree of 23.9%, a cool spot is discovered on the less massive component. Orbital period analysis indicates that the period of V1320 Cas is decreasing at a rate of dPdt=1.78×107 day yr−1, superimposed with a cyclic modulation with a period of 1.425 yr, long-term period decrease may be caused by the combination of mass transfer and angular momentum loss, and the cyclic modulation may be caused by the third companion. Using the photometric solutions and Gaia distance, we calculated the absolute physical parameters and plotted mass-luminosity and mass–radius diagrams to analyze the evolutionary status of V1320 Cas, the more massive component is a main sequence star, while the less massive component has higher luminosity and radius than those of main sequence stars with the same mass. With the decreasing orbital period, the two components of V1320 Cas will be gradually closer, while the binary may evolve toward deep contact.

我们分析了日全食接触双星V1320 Cas的光变曲线,获得了可靠的光度解,确认它是一颗W型接触双星,质量比为3.404,接触度为23.9%,在质量较小的部分发现了一个冷斑。轨道周期分析表明,V1320 Cas的周期以dPdt=1.78×10-7 day yr-1的速率下降,并叠加有周期为1.425年的周期调制,长期周期下降可能是由质量转移和角动量损失共同引起的,而周期调制可能是由第三伴星引起的。利用测光解和盖亚距离,我们计算了V1320 Cas的绝对物理参数,并绘制了质量-光度图和质量-半径图,分析了V1320 Cas的演化状况,其中质量较大的部分是一颗主序星,而质量较小的部分的光度和半径都高于相同质量的主序星。随着轨道周期的减小,V1320 Cas 的两部分会逐渐靠近,而双星可能会向深度接触演化。
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引用次数: 0
Sloshing cold fronts in galaxy cluster Abell 2566 阿贝尔2566星系团中的荡漾冷锋
IF 2 4区 物理与天体物理 Q2 ASTRONOMY & ASTROPHYSICS Pub Date : 2024-05-28 DOI: 10.1016/j.newast.2024.102253
S.K. Kadam , S.S. Sonkamble , N.D. Vagshette , M.K. Patil

This paper presents properties of the intracluster medium (ICM) in the environment of a cool core cluster Abell 2566 (redshift z = 0.08247) based on the analysis of 20 ks Chandra X-ray data. 2D imaging analysis of the Chandra data from this cluster revealed spiral structures in the morphology of X-ray emission from within the central 109 kpc formed due to gas sloshing. This analysis also witness sharp edges in the surface brightness distribution along the south-east and north-west of the X-ray peaks at 41.6 kpc and 77.4 kpc, respectively. Spectral analysis of 0.5 – 7 keV X-ray photons along these discontinuities exhibited sharp temperature jumps from 2.3 to 3.1 keV and 1.8 to 2.8 keV, respectively, with consistency in the pressure profiles, implying their association with cold fronts due to gas sloshing of the gas. Further confirmation for such an association was provided by the deprojected broken power-law density function fit to the surface brightness distribution along these wedge shaped sectorial regions. This study also witness an offset of 4.6  (6.8 kpc) between the BCG and the X-ray peak, and interaction of the BCG with a sub-system in the central region, pointing towards the origin of the spiral structure due to a minor merger.

本文根据对 20 ks 钱德拉 X 射线数据的分析,介绍了冷核星团 Abell 2566(红移 z = 0.08247)环境中星团内介质(ICM)的特性。对该星团的钱德拉数据进行的二维成像分析表明,在中心 109 kpc 范围内的 X 射线辐射形态中,存在着由于气体荡动而形成的螺旋结构。该分析还发现,在 41.6 kpc 和 77.4 kpc 的 X 射线峰值的东南和西北方向,表面亮度分布存在尖锐的边缘。对沿这些不连续面的 0.5-7 千伏 X 射线光子进行的光谱分析显示,温度分别从 2.3 千伏跃升到 3.1 千伏,从 1.8 千伏跃升到 2.8 千伏,而且压力剖面一致,这意味着它们与气体荡动引起的冷锋有关。对这些楔形扇形区域的表面亮度分布进行的破碎幂律密度函数拟合进一步证实了这种关联。这项研究还发现 BCG 与 X 射线峰之间存在 4.6′′(6.8 kpc)的偏移,BCG 与中心区域的一个子系统发生了相互作用,这表明螺旋结构的起源是由于一次小规模合并造成的。
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引用次数: 0
Effects of expansion-free condition on adiabatic collapse in f(G,T) gravity 无膨胀条件对 f(G,T) 引力绝热塌缩的影响
IF 2 4区 物理与天体物理 Q2 ASTRONOMY & ASTROPHYSICS Pub Date : 2024-05-28 DOI: 10.1016/j.newast.2024.102256
Riaz Ahmed

This study explores the impact of f(G,T) gravity, where G is the Gauss Bonnet invariant and T is the trace of the energy–momentum tensor, on the adiabatic anisotropic spherical gravitating source under the expansion-free condition. We coupled the relativistic matter with spherical symmetric structure by applying f(G,T)=αGn+λT Gauss–Bonnet model with a linear trace. To derive the collapse equation, we used the perturbation method on the field equations and the contracted Bianchi identities. The dynamics of instability range is depicted in Newtonian (N) and post-Newtonian (pN) regimes. Furthermore, instead of using the adiabatic index, we establish the instability range by looking at the density profile and anisotropic pressure configuration. We investigate the analytic solutions that meets the expansion-free condition. Finally, we have successfully achieved the original results obtained by Herrera et al. (2012) in General Relativity by setting α=λ=0 in proposed cosmological model.

本研究探讨了 f(G,T) 引力在无膨胀条件下对绝热各向异性球形引力源的影响,其中 G 是高斯-波奈不变式,T 是能动张量的迹。我们采用 f(G,T)=αGn+λT 高斯-波内特模型与线性迹线将相对论物质与球对称结构耦合。为了推导坍缩方程,我们使用了场方程的扰动法和收缩的比安奇等式。在牛顿(N)和后牛顿(pN)状态下描述了不稳定范围的动力学。此外,我们不使用绝热指数,而是通过观察密度剖面和各向异性压力配置来确定不稳定范围。我们研究了满足无膨胀条件的解析解。最后,我们在提出的宇宙学模型中设定α=λ=0,成功地实现了埃雷拉等人(2012)在广义相对论中获得的原始结果。
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引用次数: 0
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