In the present work we analyze a dynamical wormhole solution with two fluids system (one isotropic and homogeneous and the other being inhomogeneous and anisotropic in nature) as the matter at the throat. We choose two different forms of Equation of State(EoS) and investigate two solutions of the wormhole geometry. The properties to ensure existence and traversability has been analyzed. Also, the model of the dynamic wormhole has been examined for a possibility of the Emergent Universe(EU) model in cosmological context. Finally, for the dynamical wormholes so obtained, Null Energy Condition(NEC) has been examined near the throat.
{"title":"Does dynamical wormhole evolve from emergent scenario?","authors":"Dhritimalya Roy , Ayanendu Dutta , Bikram Ghosh , Subenoy Chakraborty","doi":"10.1016/j.newast.2024.102248","DOIUrl":"https://doi.org/10.1016/j.newast.2024.102248","url":null,"abstract":"<div><p>In the present work we analyze a dynamical wormhole solution with two fluids system (one isotropic and homogeneous and the other being inhomogeneous and anisotropic in nature) as the matter at the throat. We choose two different forms of Equation of State(EoS) and investigate two solutions of the wormhole geometry. The properties to ensure existence and traversability has been analyzed. Also, the model of the dynamic wormhole has been examined for a possibility of the Emergent Universe(EU) model in cosmological context. Finally, for the dynamical wormholes so obtained, Null Energy Condition(NEC) has been examined near the throat.</p></div>","PeriodicalId":54727,"journal":{"name":"New Astronomy","volume":"111 ","pages":"Article 102248"},"PeriodicalIF":2.0,"publicationDate":"2024-05-06","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140894097","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}
Pub Date : 2024-05-04DOI: 10.1016/j.newast.2024.102246
Meenu Prajapati, Mamta Gulati
Stellar orbits and the evolution of galaxies are intertwined processes that have long-term implications on each other. This paper studies how stellar orbits at the galaxy’s central region are disturbed by an asymmetric dark matter halo potential. Evidence from the observations and simulations in the Milky Way type galaxy suggests that the center of the dark matter halo could be off-centered by a few parsecs concerning the center of the core. The equations of motion of stars in the core of galaxies are expressed in terms of three-dimensional perturbed potential arising from the offset halo. The central region’s azimuthal variation in the effective potential is obtained and the first-order epicyclic theory is used to solve for the orbits. The magnitude of this perturbation potential grows at small radii and exhibits azimuthal fluctuations. In the central region, within 3 kpc radius, even a small halo offset of 300 pc can cause a surprisingly strong spatial and kinematical lopsidedness. A planar orbit, initially assumed to be in disc plane, tends to leave the plane giving rise to non-planar configuration. Furthermore, as long as the halo offset persists, the central region will stay lopsided. The dark matter halo would significantly impact the dynamic development of this region and could help fuel the active galactic nucleus.
恒星轨道和星系演化是相互交织的过程,对彼此都有长期影响。本文研究了星系中心区域的恒星轨道如何受到不对称暗物质光环势能的干扰。在银河系中的观测和模拟证据表明,暗物质晕的中心可能与核心中心偏离几帕斯卡。星系核心恒星的运动方程是用偏移光环产生的三维扰动势来表示的。得到了中心区域有效位势的方位角变化,并利用一阶外圆理论求解了轨道。这种扰动势的大小在小半径处增长,并表现出 m=1 的方位角波动。在半径为 3 kpc 的中心区域,即使是 300 pc 的微小光环偏移,也会造成令人惊讶的强烈空间和运动学倾斜。最初假定在圆盘平面内的平面轨道往往会离开平面,从而产生非平面构型。此外,只要光环偏移持续存在,中心区域就会保持倾斜。暗物质光环将对这一区域的动态发展产生重大影响,并可能为活动星系核提供燃料。
{"title":"Three-dimensional stellar orbits due to off-centered dark matter halo at the center of the disc galaxies","authors":"Meenu Prajapati, Mamta Gulati","doi":"10.1016/j.newast.2024.102246","DOIUrl":"https://doi.org/10.1016/j.newast.2024.102246","url":null,"abstract":"<div><p>Stellar orbits and the evolution of galaxies are intertwined processes that have long-term implications on each other. This paper studies how stellar orbits at the galaxy’s central region are disturbed by an asymmetric dark matter halo potential. Evidence from the observations and simulations in the Milky Way type galaxy suggests that the center of the dark matter halo could be off-centered by a few parsecs concerning the center of the core. The equations of motion of stars in the core of galaxies are expressed in terms of three-dimensional perturbed potential arising from the offset halo. The central region’s azimuthal variation in the effective potential is obtained and the first-order epicyclic theory is used to solve for the orbits. The magnitude of this perturbation potential grows at small radii and exhibits <span><math><mrow><mi>m</mi><mo>=</mo><mn>1</mn></mrow></math></span> azimuthal fluctuations. In the central region, within 3 kpc radius, even a small halo offset of 300 pc can cause a surprisingly strong spatial and kinematical lopsidedness. A planar orbit, initially assumed to be in disc plane, tends to leave the plane giving rise to non-planar configuration. Furthermore, as long as the halo offset persists, the central region will stay lopsided. The dark matter halo would significantly impact the dynamic development of this region and could help fuel the active galactic nucleus.</p></div>","PeriodicalId":54727,"journal":{"name":"New Astronomy","volume":"111 ","pages":"Article 102246"},"PeriodicalIF":2.0,"publicationDate":"2024-05-04","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140894096","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}
Pub Date : 2024-04-30DOI: 10.1016/j.newast.2024.102247
Euaggelos E. Zotos , Christof Jung
We study the dynamics in the outer regions of a rotating barred galaxy and in particular, we observe the escape of a test particle from the gravitational potential of the galaxy. The acceleration mechanism of the test particle is a close encounter with one of the ends of the bar with the right relative phase of the position of the bar. This is a possible mechanism for the creation of high-velocity stars, i.e. stars with an energy sufficient to escape from the galaxy. Our results suggest that good candidates for high-velocity stars accelerated by this mechanism are the old low-mass high-velocity stars moving close to the disc. We will encounter the asymptotic dynamics which leads naturally to the study of a type of Poincaré map which can be reinterpreted as a scattering map. Thereby an iterated scattering map enters the picture in a quite natural form. The present work is a supplement to previous work on the dynamics in the inner region of the same model.
{"title":"Escape from a rotating barred galaxy","authors":"Euaggelos E. Zotos , Christof Jung","doi":"10.1016/j.newast.2024.102247","DOIUrl":"https://doi.org/10.1016/j.newast.2024.102247","url":null,"abstract":"<div><p>We study the dynamics in the outer regions of a rotating barred galaxy and in particular, we observe the escape of a test particle from the gravitational potential of the galaxy. The acceleration mechanism of the test particle is a close encounter with one of the ends of the bar with the right relative phase of the position of the bar. This is a possible mechanism for the creation of high-velocity stars, i.e. stars with an energy sufficient to escape from the galaxy. Our results suggest that good candidates for high-velocity stars accelerated by this mechanism are the old low-mass high-velocity stars moving close to the disc. We will encounter the asymptotic dynamics which leads naturally to the study of a type of Poincaré map which can be reinterpreted as a scattering map. Thereby an iterated scattering map enters the picture in a quite natural form. The present work is a supplement to previous work on the dynamics in the inner region of the same model.</p></div>","PeriodicalId":54727,"journal":{"name":"New Astronomy","volume":"111 ","pages":"Article 102247"},"PeriodicalIF":2.0,"publicationDate":"2024-04-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140879440","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}
Pub Date : 2024-04-25DOI: 10.1016/j.newast.2024.102234
Ping Li, Wen-Ping Liao, Qi-Huan Zeng, Qi-Bin Sun, Min-Yu Li
<div><p>We model the TESS light curve of the binary system RX Dra, and also first calculate a lot of theoretical models to fit the g-mode frequencies previously detected from the TESS series of this system. The mass ratio is determined to be <span><math><mi>q</mi></math></span>=0.9026<span><math><msubsup><mrow></mrow><mrow><mo>−</mo><mn>0</mn><mo>.</mo><mn>0032</mn></mrow><mrow><mo>+</mo><mn>0</mn><mo>.</mo><mn>0032</mn></mrow></msubsup></math></span>. We newly found that there are 16 frequencies (F1–F7, F11–F20) identified as dipole g-modes, two frequencies (F21, F22) identified as quadrupole g-modes, and another two frequencies (F23, F24) identified as g-sextupole modes, based on these model fits. The primary star is newly determined to be a <span><math><mi>γ</mi></math></span> Dor pulsator in the main-sequence stage with a rotation period of about 5.7<span><math><msubsup><mrow></mrow><mrow><mo>−</mo><mn>0</mn><mo>.</mo><mn>2</mn></mrow><mrow><mo>+</mo><mn>0</mn><mo>.</mo><mn>7</mn></mrow></msubsup></math></span> days, rotating slower than the orbital motion. The fundamental parameters of two components are firstly estimated as follows: <span><math><msub><mrow><mi>M</mi></mrow><mrow><mn>1</mn></mrow></msub></math></span>=1.53<span><math><msubsup><mrow></mrow><mrow><mo>−</mo><mn>0</mn><mo>.</mo><mn>17</mn></mrow><mrow><mo>+</mo><mn>0</mn><mo>.</mo><mn>00</mn></mrow></msubsup></math></span> M <span><math><msub><mrow></mrow><mrow><mo>⊙</mo></mrow></msub></math></span>, <span><math><msub><mrow><mi>M</mi></mrow><mrow><mn>2</mn></mrow></msub></math></span>= 1.38<span><math><msubsup><mrow></mrow><mrow><mo>−</mo><mn>0</mn><mo>.</mo><mn>00</mn></mrow><mrow><mo>+</mo><mn>0</mn><mo>.</mo><mn>18</mn></mrow></msubsup></math></span> M <span><math><msub><mrow></mrow><mrow><mo>⊙</mo></mrow></msub></math></span>, <span><math><msub><mrow><mi>T</mi></mrow><mrow><mn>1</mn></mrow></msub></math></span>=7240<span><math><msubsup><mrow></mrow><mrow><mo>−</mo><mn>44</mn></mrow><mrow><mo>+</mo><mn>490</mn></mrow></msubsup></math></span> K, <span><math><msub><mrow><mi>T</mi></mrow><mrow><mn>2</mn></mrow></msub></math></span>=6747<span><math><msubsup><mrow></mrow><mrow><mo>−</mo><mn>221</mn></mrow><mrow><mo>+</mo><mn>201</mn></mrow></msubsup></math></span> K, <span><math><msub><mrow><mi>R</mi></mrow><mrow><mn>1</mn></mrow></msub></math></span>=1.8288<span><math><msubsup><mrow></mrow><mrow><mo>−</mo><mn>0</mn><mo>.</mo><mn>0959</mn></mrow><mrow><mo>+</mo><mn>0</mn><mo>.</mo><mn>0260</mn></mrow></msubsup></math></span> R <span><math><msub><mrow></mrow><mrow><mo>⊙</mo></mrow></msub></math></span>, <span><math><msub><mrow><mi>R</mi></mrow><mrow><mn>2</mn></mrow></msub></math></span>= 1.3075<span><math><msubsup><mrow></mrow><mrow><mo>−</mo><mn>0</mn><mo>.</mo><mn>2543</mn></mrow><mrow><mo>+</mo><mn>0</mn><mo>.</mo><mn>0450</mn></mrow></msubsup></math></span> R <span><math><msub><mrow></mrow><mrow><mo>⊙</mo></mrow></msub></math></span>, <span><math><msub><mrow><mi>L</mi></mrow><
我们对双星系统 RX Dra 的 TESS 光曲线进行了建模,并首先计算了大量理论模型,以拟合之前从该系统的 TESS 系列中探测到的 g 模式频率。质量比被确定为q=0.9026-0.0032+0.0032。根据这些模型拟合,我们新发现有 16 个频率(F1-F7,F11-F20)被确定为偶极 g 模式,两个频率(F21,F22)被确定为四极 g 模式,另外两个频率(F23,F24)被确定为 g 六极模式。新测定的主星是一颗处于主序阶段的γ Dor 脉动器,自转周期约为 5.7-0.2+0.7 天,自转速度慢于轨道运动。首先估算出两个分量的基本参数如下m1=1.53-0.17+0.00 m ⊙, m2=1.38-0.00+0.18 m ⊙, t1=7240-44+490 k, t2=6747-221+201 k, r1=1.8288-0.0959+0.0260 R ⊙,R2= 1.3075-0.2543+0.0450 R ⊙,L1=8.2830-0.6036+1.8015 L ⊙,L2=3.4145-0.1843+0.1320 L ⊙。我们的结果表明,这颗次星位于 H-R 图中的类太阳脉动器区域,表明它可能是这一类型的脉动星。最后,主星对流核心的半径估计约为 0.1403-0.0000+0.0206 R ⊙。
{"title":"Exploring the physical properties of the γ Dor binary star RX Dra with photometry and asteroseismology","authors":"Ping Li, Wen-Ping Liao, Qi-Huan Zeng, Qi-Bin Sun, Min-Yu Li","doi":"10.1016/j.newast.2024.102234","DOIUrl":"10.1016/j.newast.2024.102234","url":null,"abstract":"<div><p>We model the TESS light curve of the binary system RX Dra, and also first calculate a lot of theoretical models to fit the g-mode frequencies previously detected from the TESS series of this system. The mass ratio is determined to be <span><math><mi>q</mi></math></span>=0.9026<span><math><msubsup><mrow></mrow><mrow><mo>−</mo><mn>0</mn><mo>.</mo><mn>0032</mn></mrow><mrow><mo>+</mo><mn>0</mn><mo>.</mo><mn>0032</mn></mrow></msubsup></math></span>. We newly found that there are 16 frequencies (F1–F7, F11–F20) identified as dipole g-modes, two frequencies (F21, F22) identified as quadrupole g-modes, and another two frequencies (F23, F24) identified as g-sextupole modes, based on these model fits. The primary star is newly determined to be a <span><math><mi>γ</mi></math></span> Dor pulsator in the main-sequence stage with a rotation period of about 5.7<span><math><msubsup><mrow></mrow><mrow><mo>−</mo><mn>0</mn><mo>.</mo><mn>2</mn></mrow><mrow><mo>+</mo><mn>0</mn><mo>.</mo><mn>7</mn></mrow></msubsup></math></span> days, rotating slower than the orbital motion. The fundamental parameters of two components are firstly estimated as follows: <span><math><msub><mrow><mi>M</mi></mrow><mrow><mn>1</mn></mrow></msub></math></span>=1.53<span><math><msubsup><mrow></mrow><mrow><mo>−</mo><mn>0</mn><mo>.</mo><mn>17</mn></mrow><mrow><mo>+</mo><mn>0</mn><mo>.</mo><mn>00</mn></mrow></msubsup></math></span> M <span><math><msub><mrow></mrow><mrow><mo>⊙</mo></mrow></msub></math></span>, <span><math><msub><mrow><mi>M</mi></mrow><mrow><mn>2</mn></mrow></msub></math></span>= 1.38<span><math><msubsup><mrow></mrow><mrow><mo>−</mo><mn>0</mn><mo>.</mo><mn>00</mn></mrow><mrow><mo>+</mo><mn>0</mn><mo>.</mo><mn>18</mn></mrow></msubsup></math></span> M <span><math><msub><mrow></mrow><mrow><mo>⊙</mo></mrow></msub></math></span>, <span><math><msub><mrow><mi>T</mi></mrow><mrow><mn>1</mn></mrow></msub></math></span>=7240<span><math><msubsup><mrow></mrow><mrow><mo>−</mo><mn>44</mn></mrow><mrow><mo>+</mo><mn>490</mn></mrow></msubsup></math></span> K, <span><math><msub><mrow><mi>T</mi></mrow><mrow><mn>2</mn></mrow></msub></math></span>=6747<span><math><msubsup><mrow></mrow><mrow><mo>−</mo><mn>221</mn></mrow><mrow><mo>+</mo><mn>201</mn></mrow></msubsup></math></span> K, <span><math><msub><mrow><mi>R</mi></mrow><mrow><mn>1</mn></mrow></msub></math></span>=1.8288<span><math><msubsup><mrow></mrow><mrow><mo>−</mo><mn>0</mn><mo>.</mo><mn>0959</mn></mrow><mrow><mo>+</mo><mn>0</mn><mo>.</mo><mn>0260</mn></mrow></msubsup></math></span> R <span><math><msub><mrow></mrow><mrow><mo>⊙</mo></mrow></msub></math></span>, <span><math><msub><mrow><mi>R</mi></mrow><mrow><mn>2</mn></mrow></msub></math></span>= 1.3075<span><math><msubsup><mrow></mrow><mrow><mo>−</mo><mn>0</mn><mo>.</mo><mn>2543</mn></mrow><mrow><mo>+</mo><mn>0</mn><mo>.</mo><mn>0450</mn></mrow></msubsup></math></span> R <span><math><msub><mrow></mrow><mrow><mo>⊙</mo></mrow></msub></math></span>, <span><math><msub><mrow><mi>L</mi></mrow><","PeriodicalId":54727,"journal":{"name":"New Astronomy","volume":"111 ","pages":"Article 102234"},"PeriodicalIF":2.0,"publicationDate":"2024-04-25","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140791345","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}
Pub Date : 2024-04-23DOI: 10.1016/j.newast.2024.102245
Faizuddin Ahmed
In this paper, we exploration a Petrov type-N vacuum solution to Einstein’s field equations, while incorporating a negative cosmological constant () within the framework of modified gravity theories. This solution intriguingly accommodates closed time-like curves at a particular moment in time, effectively violates the causality condition, thus acts as a time-machine model. A key observation is that the determinant of the Ricci tensor for this particular Einstein space metric differs from zero. This noteworthy finding suggests to the existence of an anti-curvature tensor defined and hence, an anti-curvature scalar , which is introduced with the Lagrangian of the system, thereby giving rise to as Ricci-inverse gravity theory. We consider class-I models of Ricci-inverse gravity, where the function with is the coupling constant. We demonstrate that this Einstein space metric serves as a vacuum solution with a negative modified cosmological constant within the framework of Ricci-inverse gravity. Consequently, the violation of causality persists within this new gravity theory as well. Moreover, we solve the modified field equations by considering matter content other than vacuum and demonstrate that the energy-density and isotropic pressure satisfies the equation .
{"title":"f(R,A) gravity theory in Einstein space background and causality violation","authors":"Faizuddin Ahmed","doi":"10.1016/j.newast.2024.102245","DOIUrl":"10.1016/j.newast.2024.102245","url":null,"abstract":"<div><p>In this paper, we exploration a Petrov type-N vacuum solution to Einstein’s field equations, while incorporating a negative cosmological constant (<span><math><mrow><mi>Λ</mi><mo><</mo><mn>0</mn></mrow></math></span>) within the framework of modified gravity theories. This solution intriguingly accommodates closed time-like curves at a particular moment in time, effectively violates the causality condition, thus acts as a time-machine model. A key observation is that the determinant of the Ricci tensor <span><math><msup><mrow><mi>R</mi></mrow><mrow><mi>μ</mi><mi>ν</mi></mrow></msup></math></span> for this particular Einstein space metric differs from zero. This noteworthy finding suggests to the existence of an anti-curvature tensor defined <span><math><mrow><msup><mrow><mi>A</mi></mrow><mrow><mi>μ</mi><mi>ν</mi></mrow></msup><mo>=</mo><msubsup><mrow><mi>R</mi></mrow><mrow><mi>μ</mi><mi>ν</mi></mrow><mrow><mo>−</mo><mn>1</mn></mrow></msubsup></mrow></math></span> and hence, an anti-curvature scalar <span><math><mrow><mi>A</mi><mo>=</mo><msub><mrow><mi>g</mi></mrow><mrow><mi>μ</mi><mi>ν</mi></mrow></msub><mspace></mspace><msup><mrow><mi>A</mi></mrow><mrow><mi>μ</mi><mi>ν</mi></mrow></msup></mrow></math></span>, which is introduced with the Lagrangian of the system, thereby giving rise to as Ricci-inverse gravity theory. We consider <strong>class-I</strong> models of Ricci-inverse gravity, where the function <span><math><mrow><mi>f</mi><mo>=</mo><mi>f</mi><mrow><mo>(</mo><mi>R</mi><mo>,</mo><mi>A</mi><mo>)</mo></mrow><mo>=</mo><mrow><mo>(</mo><mi>R</mi><mo>+</mo><mi>κ</mi><mspace></mspace><mi>A</mi><mo>)</mo></mrow></mrow></math></span> with <span><math><mi>κ</mi></math></span> is the coupling constant. We demonstrate that this Einstein space metric serves as a vacuum solution with a negative modified cosmological constant within the framework of Ricci-inverse gravity. Consequently, the violation of causality persists within this new gravity theory as well. Moreover, we solve the modified field equations by considering matter content other than vacuum and demonstrate that the energy-density and isotropic pressure satisfies the equation <span><math><mrow><mi>ρ</mi><mo>=</mo><mo>−</mo><mi>p</mi><mo>=</mo><mfrac><mrow><mn>3</mn><mspace></mspace><mi>κ</mi></mrow><mrow><mi>Λ</mi></mrow></mfrac></mrow></math></span>.</p></div>","PeriodicalId":54727,"journal":{"name":"New Astronomy","volume":"111 ","pages":"Article 102245"},"PeriodicalIF":2.0,"publicationDate":"2024-04-23","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140778925","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}
Pub Date : 2024-04-20DOI: 10.1016/j.newast.2024.102244
Suhail Masda
<div><p>We present the fundamental stellar parameters, including the individual component masses, as well as the orbital parameters, and dynamical parallaxes of the two close binary stars; HD<!--> <!-->80671, and HD<!--> <!-->97038. The stellar parameters are spectrophotometrically estimated via Al-Wardat’s method for analyzing binary and multiple stellar systems, which is having a combination of the spectroscopic analysis and the photometric analysis to build the combined and individual synthetic spectral energy distributions of the individual components of the systems and so to estimate their fundamental parameters, metallicities, and ages. It employs Kurucz’s model atmospheres of single stars, while the orbital parameters are estimated using Tokovinin’s method. The individual spectrophotometric component masses are inferred with good accuracy, and found to be <span><math><msubsup><mrow><mi>M</mi></mrow><mrow><mi>S</mi><mi>p</mi><mi>h</mi></mrow><mrow><mi>A</mi></mrow></msubsup></math></span> = 1.47<span><math><mrow><mo>±</mo><mn>0</mn><mo>.</mo><mn>10</mn><msub><mrow><mi>M</mi></mrow><mrow><mo>⊙</mo></mrow></msub></mrow></math></span> and <span><math><mrow><msubsup><mrow><mi>M</mi></mrow><mrow><mi>S</mi><mi>p</mi><mi>h</mi></mrow><mrow><mi>B</mi></mrow></msubsup><mo>=</mo><mn>1</mn><mo>.</mo><mn>29</mn><mo>±</mo><mn>0</mn><mo>.</mo><mn>09</mn><mspace></mspace><msub><mrow><mi>M</mi></mrow><mrow><mo>⊙</mo></mrow></msub></mrow></math></span> with an age of <span><math><mrow><mn>1</mn><mo>.</mo><mn>0</mn><mo>±</mo><mn>0</mn><mo>.</mo><mn>09</mn></mrow></math></span> Gyr for HD<!--> <!-->80671, and <span><math><mrow><msubsup><mrow><mi>M</mi></mrow><mrow><mi>S</mi><mi>p</mi><mi>h</mi></mrow><mrow><mi>A</mi></mrow></msubsup><mo>=</mo><mn>1</mn><mo>.</mo><mn>17</mn><mo>±</mo><mn>0</mn><mo>.</mo><mn>09</mn><mspace></mspace><msub><mrow><mi>M</mi></mrow><mrow><mo>⊙</mo></mrow></msub></mrow></math></span> and <span><math><mrow><msubsup><mrow><mi>M</mi></mrow><mrow><mi>S</mi><mi>p</mi><mi>h</mi></mrow><mrow><mi>B</mi></mrow></msubsup><mo>=</mo><mn>1</mn><mo>.</mo><mn>12</mn><mo>±</mo><mn>0</mn><mo>.</mo><mn>08</mn><mspace></mspace><msub><mrow><mi>M</mi></mrow><mrow><mo>⊙</mo></mrow></msub></mrow></math></span> with an age of <span><math><mrow><mn>3</mn><mo>.</mo><mn>981</mn><mo>±</mo><mn>0</mn><mo>.</mo><mn>35</mn></mrow></math></span> Gyr for HD<!--> <!-->97038. The improved dynamical parallaxes are given as <span><math><mrow><msub><mrow><mi>π</mi></mrow><mrow><mi>d</mi><mi>y</mi><mi>n</mi></mrow></msub><mo>=</mo><mn>28</mn><mo>.</mo><mn>305</mn><mo>±</mo><mn>0</mn><mo>.</mo><mn>45</mn></mrow></math></span> mas for HD<!--> <!-->80671, and <span><math><mrow><msub><mrow><mi>π</mi></mrow><mrow><mi>d</mi><mi>y</mi><mi>n</mi></mrow></msub><mo>=</mo><mn>16</mn><mo>.</mo><mn>26</mn><mo>±</mo><mn>0</mn><mo>.</mo><mn>30</mn></mrow></math></span> mas for HD<!--> <!-->97038. The evolutionary status of two binaries is discussed depending on the positions of the compo
{"title":"The improved component masses and parallaxes for the two close binary stars: HD 80671 and HD 97038","authors":"Suhail Masda","doi":"10.1016/j.newast.2024.102244","DOIUrl":"10.1016/j.newast.2024.102244","url":null,"abstract":"<div><p>We present the fundamental stellar parameters, including the individual component masses, as well as the orbital parameters, and dynamical parallaxes of the two close binary stars; HD<!--> <!-->80671, and HD<!--> <!-->97038. The stellar parameters are spectrophotometrically estimated via Al-Wardat’s method for analyzing binary and multiple stellar systems, which is having a combination of the spectroscopic analysis and the photometric analysis to build the combined and individual synthetic spectral energy distributions of the individual components of the systems and so to estimate their fundamental parameters, metallicities, and ages. It employs Kurucz’s model atmospheres of single stars, while the orbital parameters are estimated using Tokovinin’s method. The individual spectrophotometric component masses are inferred with good accuracy, and found to be <span><math><msubsup><mrow><mi>M</mi></mrow><mrow><mi>S</mi><mi>p</mi><mi>h</mi></mrow><mrow><mi>A</mi></mrow></msubsup></math></span> = 1.47<span><math><mrow><mo>±</mo><mn>0</mn><mo>.</mo><mn>10</mn><msub><mrow><mi>M</mi></mrow><mrow><mo>⊙</mo></mrow></msub></mrow></math></span> and <span><math><mrow><msubsup><mrow><mi>M</mi></mrow><mrow><mi>S</mi><mi>p</mi><mi>h</mi></mrow><mrow><mi>B</mi></mrow></msubsup><mo>=</mo><mn>1</mn><mo>.</mo><mn>29</mn><mo>±</mo><mn>0</mn><mo>.</mo><mn>09</mn><mspace></mspace><msub><mrow><mi>M</mi></mrow><mrow><mo>⊙</mo></mrow></msub></mrow></math></span> with an age of <span><math><mrow><mn>1</mn><mo>.</mo><mn>0</mn><mo>±</mo><mn>0</mn><mo>.</mo><mn>09</mn></mrow></math></span> Gyr for HD<!--> <!-->80671, and <span><math><mrow><msubsup><mrow><mi>M</mi></mrow><mrow><mi>S</mi><mi>p</mi><mi>h</mi></mrow><mrow><mi>A</mi></mrow></msubsup><mo>=</mo><mn>1</mn><mo>.</mo><mn>17</mn><mo>±</mo><mn>0</mn><mo>.</mo><mn>09</mn><mspace></mspace><msub><mrow><mi>M</mi></mrow><mrow><mo>⊙</mo></mrow></msub></mrow></math></span> and <span><math><mrow><msubsup><mrow><mi>M</mi></mrow><mrow><mi>S</mi><mi>p</mi><mi>h</mi></mrow><mrow><mi>B</mi></mrow></msubsup><mo>=</mo><mn>1</mn><mo>.</mo><mn>12</mn><mo>±</mo><mn>0</mn><mo>.</mo><mn>08</mn><mspace></mspace><msub><mrow><mi>M</mi></mrow><mrow><mo>⊙</mo></mrow></msub></mrow></math></span> with an age of <span><math><mrow><mn>3</mn><mo>.</mo><mn>981</mn><mo>±</mo><mn>0</mn><mo>.</mo><mn>35</mn></mrow></math></span> Gyr for HD<!--> <!-->97038. The improved dynamical parallaxes are given as <span><math><mrow><msub><mrow><mi>π</mi></mrow><mrow><mi>d</mi><mi>y</mi><mi>n</mi></mrow></msub><mo>=</mo><mn>28</mn><mo>.</mo><mn>305</mn><mo>±</mo><mn>0</mn><mo>.</mo><mn>45</mn></mrow></math></span> mas for HD<!--> <!-->80671, and <span><math><mrow><msub><mrow><mi>π</mi></mrow><mrow><mi>d</mi><mi>y</mi><mi>n</mi></mrow></msub><mo>=</mo><mn>16</mn><mo>.</mo><mn>26</mn><mo>±</mo><mn>0</mn><mo>.</mo><mn>30</mn></mrow></math></span> mas for HD<!--> <!-->97038. The evolutionary status of two binaries is discussed depending on the positions of the compo","PeriodicalId":54727,"journal":{"name":"New Astronomy","volume":"111 ","pages":"Article 102244"},"PeriodicalIF":2.0,"publicationDate":"2024-04-20","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140772694","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}
Pub Date : 2024-04-17DOI: 10.1016/j.newast.2024.102235
Ai-Ying Zhou
Using the TESS and Kepler K2 light curve archives, I have reanalyzed 13 known Scuti stars. AD Ari is now reclassified as a rotating ellipsoidal binary variable. EX Cnc and HD 73712 are reclassified as hybrid Sct- Dor pulsators. EX Cnc turns out to be an enticing asteroseismic target because of its three distinct groups of pulsation frequencies. The strong beating caused by two close frequencies is present in the star CD-54 7154. More than 71 pulsation frequencies were resolved for Boo and IT Dra with high significant levels, while V1821 Cyg, V2238 Cyg, BR Cnc, BU Cnc, and BV Cnc pulsate with a few dozen frequencies. In particular, K2 data revealed a significantly richer pulsational spectrum for the two Scuti stars BU Cnc and BV Cnc from six to 26. Unlike the other 12 stars, BN Cnc shows the simplest pulsation pattern. With high-precision and long-term space-based photometry, we are able to discern the pulsational contents of these stars more clearly and enhance our knowledge of them. This reanalysis using TESS and Kepler K2 data highlights the diversity of pulsational behavior among Scuti stars and the value of long-duration, high-precision photometry. Further asteroseismic modeling of these stars, particularly EX Cnc with its distinct frequency groups, promises to refine our understanding of their internal structures and pulsational mechanisms.
{"title":"Resolving the pulsation contents of 13 δ Scuti stars with TESS and K2","authors":"Ai-Ying Zhou","doi":"10.1016/j.newast.2024.102235","DOIUrl":"https://doi.org/10.1016/j.newast.2024.102235","url":null,"abstract":"<div><p>Using the <em>TESS</em> and <em>Kepler</em> K2 light curve archives, I have reanalyzed 13 known <span><math><mi>δ</mi></math></span> Scuti stars. AD Ari is now reclassified as a rotating ellipsoidal binary variable. EX Cnc and HD 73712 are reclassified as hybrid <span><math><mi>δ</mi></math></span> Sct-<span><math><mi>γ</mi></math></span> Dor pulsators. EX Cnc turns out to be an enticing asteroseismic target because of its three distinct groups of pulsation frequencies. The strong beating caused by two close frequencies is present in the star CD-54 7154. More than 71 pulsation frequencies were resolved for <span><math><mi>ι</mi></math></span> Boo and IT Dra with high significant levels, while V1821 Cyg, V2238 Cyg, BR Cnc, BU Cnc, and BV Cnc pulsate with a few dozen frequencies. In particular, K2 data revealed a significantly richer pulsational spectrum for the two <span><math><mi>δ</mi></math></span> Scuti stars BU Cnc and BV Cnc from six to 26. Unlike the other 12 stars, BN Cnc shows the simplest pulsation pattern. With high-precision and long-term space-based photometry, we are able to discern the pulsational contents of these stars more clearly and enhance our knowledge of them. This reanalysis using <em>TESS</em> and <em>Kepler</em> K2 data highlights the diversity of pulsational behavior among <span><math><mi>δ</mi></math></span> Scuti stars and the value of long-duration, high-precision photometry. Further asteroseismic modeling of these stars, particularly EX Cnc with its distinct frequency groups, promises to refine our understanding of their internal structures and pulsational mechanisms.</p></div>","PeriodicalId":54727,"journal":{"name":"New Astronomy","volume":"111 ","pages":"Article 102235"},"PeriodicalIF":2.0,"publicationDate":"2024-04-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140646292","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}
Pub Date : 2024-04-16DOI: 10.1016/j.newast.2024.102236
Ayanendu Dutta , Dhritimalya Roy , Subenoy Chakraborty
The present work investigates the general wormhole solution in Einstein gravity with an exponential shape function around an ultrastatic and a finite redshift geometry. The geodesic motion around the wormholes is studied in which the deflection angle of the orbiting photon sphere is found to be negative after a certain region, indicating the presence of repulsive effect of gravity in both the ultrastatic and finite redshift wormholes. Various unbounded and bounded timelike trajectories are presented on the wormhole embedding diagrams, in which some of the bound orbits involve intersection points that may lead to causality violating geodesics. Another class of closed timelike geodesics are obtained in the unstable circular trajectory that appeared at the wormhole throat. Finally, the trajectories are classified in terms of the family of CTG orbits.
{"title":"Particle motion around traversable wormholes: Possibility of closed timelike geodesics","authors":"Ayanendu Dutta , Dhritimalya Roy , Subenoy Chakraborty","doi":"10.1016/j.newast.2024.102236","DOIUrl":"https://doi.org/10.1016/j.newast.2024.102236","url":null,"abstract":"<div><p>The present work investigates the general wormhole solution in Einstein gravity with an exponential shape function around an ultrastatic and a finite redshift geometry. The geodesic motion around the wormholes is studied in which the deflection angle of the orbiting photon sphere is found to be negative after a certain region, indicating the presence of repulsive effect of gravity in both the ultrastatic and finite redshift wormholes. Various unbounded and bounded timelike trajectories are presented on the wormhole embedding diagrams, in which some of the bound orbits involve intersection points that may lead to causality violating geodesics. Another class of closed timelike geodesics are obtained in the unstable circular trajectory that appeared at the wormhole throat. Finally, the trajectories are classified in terms of the family of CTG orbits.</p></div>","PeriodicalId":54727,"journal":{"name":"New Astronomy","volume":"111 ","pages":"Article 102236"},"PeriodicalIF":2.0,"publicationDate":"2024-04-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140605221","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}
Pub Date : 2024-04-13DOI: 10.1016/j.newast.2024.102233
Bin Zhang , Yidan Gao
The photometric study of the short period contact binary V415 Gem are performed for the first time. We discovered that it is a W-subtype shallow contact binary with a mass ratio of q = 2.297 and a contact degree of f = 3.6%. The light curves of the target exhibit an O’Connell effect, we attached a cool star-spot on its primary component for better fitting results. At the same time, the third light was found during our analysis by using the 2015 version of the Wilson–Devinney () code. And the average luminosity contribution of the third light is 44% of the total light. Besides, the curve of V415 Gem exhibits a cyclic variation, which is due to the light-travel time effect caused by the presence of a third component with an amplitude of 0.0033 days and a period of 11.5 years. The mass of the third body is estimated to be MM.
{"title":"The first study of the short period contact binary V415 Gem","authors":"Bin Zhang , Yidan Gao","doi":"10.1016/j.newast.2024.102233","DOIUrl":"https://doi.org/10.1016/j.newast.2024.102233","url":null,"abstract":"<div><p>The photometric study of the short period contact binary V415 Gem are performed for the first time. We discovered that it is a W-subtype shallow contact binary with a mass ratio of q = 2.297 and a contact degree of f = 3.6%. The light curves of the target exhibit an O’Connell effect, we attached a cool star-spot on its primary component for better fitting results. At the same time, the third light was found during our analysis by using the 2015 version of the Wilson–Devinney (<span><math><mrow><mi>W</mi><mo>−</mo><mi>D</mi></mrow></math></span>) code. And the average luminosity contribution of the third light is 44% of the total light. Besides, the <span><math><mrow><mi>O</mi><mo>−</mo><mi>C</mi></mrow></math></span> curve of V415 Gem exhibits a cyclic variation, which is due to the light-travel time effect caused by the presence of a third component with an amplitude of 0.0033 days and a period of 11.5 years. The mass of the third body is estimated to be M<span><math><mrow><msub><mrow></mrow><mrow><mn>3</mn></mrow></msub><mo>∼</mo><mn>1</mn><mo>.</mo><mn>08</mn></mrow></math></span>M<span><math><msub><mrow></mrow><mrow><mo>⊙</mo></mrow></msub></math></span>.</p></div>","PeriodicalId":54727,"journal":{"name":"New Astronomy","volume":"111 ","pages":"Article 102233"},"PeriodicalIF":2.0,"publicationDate":"2024-04-13","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140554673","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}
The astronomical data analysis consists of two crucial process; data reduction of the captured images and data analysis of the derived magnitudes. We present the platform ASIVA, a data analysis platform which comes along with a data reduction pipeline. The data reduction pipeline gives flexibility to analyse the FITS images and also perform image alignment for detecting the correct image coordinates for required objects. It can be custom scheduled with cron jobs so that it picks the latest data and appends the results accordingly. The data analysis platform allows user to effectively analyse the ensemble data and perform accurate data processing and grouping with ease. It is integrated with a custom algorithm to detect the variable stars from an ensemble with its relative standard deviations. The statistical, spectral and non-linear dynamics features can be extracted from time series data which can be eventually used for in-depth analysis. To validate the capability, we have analysed 15 nights of Orion Nebula Cluster field in I filter which had 1585 images. ASIVA reduces manual effort to a great extent thus saves analysis time and excludes human errors.
{"title":"ASIVA – Platform for observational and computational analysis of stellar variables","authors":"Parvej Reja Saleh , Tanveer Singh , Debasish Hazarika , Surabhi Rajkumari , Saurabh Rajkumar , Pritam Das , Padmakar Singh Parihar , Eeshankur Saikia","doi":"10.1016/j.newast.2024.102232","DOIUrl":"https://doi.org/10.1016/j.newast.2024.102232","url":null,"abstract":"<div><p>The astronomical data analysis consists of two crucial process; data reduction of the captured images and data analysis of the derived magnitudes. We present the platform ASIVA, a data analysis platform which comes along with a data reduction pipeline. The data reduction pipeline gives flexibility to analyse the FITS images and also perform image alignment for detecting the correct image coordinates for required objects. It can be custom scheduled with cron jobs so that it picks the latest data and appends the results accordingly. The data analysis platform allows user to effectively analyse the ensemble data and perform accurate data processing and grouping with ease. It is integrated with a custom algorithm to detect the variable stars from an ensemble with its relative standard deviations. The statistical, spectral and non-linear dynamics features can be extracted from time series data which can be eventually used for in-depth analysis. To validate the capability, we have analysed 15 nights of Orion Nebula Cluster field in I filter which had 1585 images. ASIVA reduces manual effort to a great extent thus saves analysis time and excludes human errors.</p></div>","PeriodicalId":54727,"journal":{"name":"New Astronomy","volume":"111 ","pages":"Article 102232"},"PeriodicalIF":2.0,"publicationDate":"2024-04-06","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140618276","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}