Pub Date : 2024-05-18DOI: 10.1016/j.newast.2024.102252
M.F. Yıldırım
The light curves (LC(s)) of the shallow contact binary (SCB(s)) IR Vir were retrieved from the TESS, Kepler (K2), ASAS, ASAS-SN, and KWS databases and comprehensively analyzed in this paper. For IR Vir, a q search was conducted to determine the mass ratio, which was found to be . The analysis indicates that IR Vir was a typical A-type W UMa. Since the determination of absolute parameters is crucial for analyzing the evolution of such systems, the masses of the bodies of IR Vir were estimated as M, M, and the radii as R, R. In the analysis of the orbital period (OP(s)) for IR Vir, it was found that the OP of IR Vir was increasing, and this value was calculated to be 0.0376 s per year. The OP increase can be explained by the conserved mass exchange between the bodies, and it can be proposed to be from the low mass body to the more one. This value was calculated as per year. Furthermore, a sinusoidal change in the OP was also identified, and it was proposed that this could be attributed to the presence of a third body or magnetic activity. Finally, to gain a better understanding of the nature of IR Vir, it was positioned in the logM logJ and HR (Hertzsprung-Russell) diagrams.
本文从 TESS、开普勒(K2)、ASAS、ASAS-SN 和 KWS 数据库中检索到了浅接触双星(SCB(s))IR Vir 的光变曲线(LC(s)),并对其进行了全面分析。对IR Vir进行了q搜索以确定其质量比,结果发现其质量比为0.371±0.008。分析表明,IR Vir 是一颗典型的 A 型 W UMa。由于绝对参数的确定对于分析这类系统的演化至关重要,因此估算出IR Vir的天体质量为M1=1.03±0.10 M⊙,M2=0.38±0.05 M⊙,半径为R1=1.16±0.06 R⊙,R2=0.73±0.04 R⊙。在对 IR Vir 的轨道周期(OP(s))进行分析时,发现 IR Vir 的 OP 在不断增加,计算得出的值为每年 0.0376 秒。OP的增加可以用天体之间的质量交换来解释,可以认为是从质量小的天体到质量大的天体。经计算,该值为每年 2.4×10-7 M⊙。此外,还发现了 OP 的正弦变化,并认为这可能是由于第三个天体或磁活动的存在。最后,为了更好地了解 IR Vir 的性质,将其置于 logMtot - logJ 和 HR(赫兹普隆-拉塞尔)图中。
{"title":"A comprehensive photometric analysis of the shallow contact binary IR Vir","authors":"M.F. Yıldırım","doi":"10.1016/j.newast.2024.102252","DOIUrl":"https://doi.org/10.1016/j.newast.2024.102252","url":null,"abstract":"<div><p>The light curves (LC(s)) of the shallow contact binary (SCB(s)) IR Vir were retrieved from the TESS, Kepler (K2), ASAS, ASAS-SN, and KWS databases and comprehensively analyzed in this paper. For IR Vir, a q search was conducted to determine the mass ratio, which was found to be <span><math><mrow><mn>0</mn><mo>.</mo><mn>371</mn><mo>±</mo><mn>0</mn><mo>.</mo><mn>008</mn></mrow></math></span>. The analysis indicates that IR Vir was a typical A-type W UMa. Since the determination of absolute parameters is crucial for analyzing the evolution of such systems, the masses of the bodies of IR Vir were estimated as <span><math><mrow><msub><mrow><mi>M</mi></mrow><mrow><mn>1</mn></mrow></msub><mo>=</mo><mn>1</mn><mo>.</mo><mn>03</mn><mo>±</mo><mn>0</mn><mo>.</mo><mn>10</mn></mrow></math></span> M<span><math><msub><mrow></mrow><mrow><mo>⊙</mo></mrow></msub></math></span>, <span><math><mrow><msub><mrow><mi>M</mi></mrow><mrow><mn>2</mn></mrow></msub><mo>=</mo><mn>0</mn><mo>.</mo><mn>38</mn><mo>±</mo><mn>0</mn><mo>.</mo><mn>05</mn></mrow></math></span> M<span><math><msub><mrow></mrow><mrow><mo>⊙</mo></mrow></msub></math></span>, and the radii as <span><math><mrow><msub><mrow><mi>R</mi></mrow><mrow><mn>1</mn></mrow></msub><mo>=</mo><mn>1</mn><mo>.</mo><mn>16</mn><mo>±</mo><mn>0</mn><mo>.</mo><mn>06</mn></mrow></math></span> R<span><math><msub><mrow></mrow><mrow><mo>⊙</mo></mrow></msub></math></span>, <span><math><mrow><msub><mrow><mi>R</mi></mrow><mrow><mn>2</mn></mrow></msub><mo>=</mo><mn>0</mn><mo>.</mo><mn>73</mn><mo>±</mo><mn>0</mn><mo>.</mo><mn>04</mn></mrow></math></span> R<span><math><msub><mrow></mrow><mrow><mo>⊙</mo></mrow></msub></math></span>. In the analysis of the orbital period (OP(s)) for IR Vir, it was found that the OP of IR Vir was increasing, and this value was calculated to be 0.0376 s per year. The OP increase can be explained by the conserved mass exchange between the bodies, and it can be proposed to be from the low mass body to the more one. This value was calculated as <span><math><mrow><mn>2</mn><mo>.</mo><mn>4</mn><mo>×</mo><mn>1</mn><msup><mrow><mn>0</mn></mrow><mrow><mo>−</mo><mn>7</mn></mrow></msup></mrow></math></span> <span><math><msub><mrow><mi>M</mi></mrow><mrow><mo>⊙</mo></mrow></msub></math></span> per year. Furthermore, a sinusoidal change in the OP was also identified, and it was proposed that this could be attributed to the presence of a third body or magnetic activity. Finally, to gain a better understanding of the nature of IR Vir, it was positioned in the logM<span><math><msub><mrow></mrow><mrow><mi>t</mi><mi>o</mi><mi>t</mi></mrow></msub></math></span> <span><math><mo>−</mo></math></span> logJ and HR (Hertzsprung-Russell) diagrams.</p></div>","PeriodicalId":54727,"journal":{"name":"New Astronomy","volume":null,"pages":null},"PeriodicalIF":2.0,"publicationDate":"2024-05-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141090384","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 : 2024-05-18DOI: 10.1016/j.newast.2024.102250
Ahmed Waqas Zubairi , Zhao Ergang , Jiajia He , Fuxing Li , Liying Zhu , Azizbek Matekov
We present light curve solution of V458 Mon firstly by using the Wilson-Devinney code. The total eclipse and deep minima of the light curves of V458 Mon enable us to determine reliable orbital parameters of the binary system. The solution suggests that V458 Mon is a low mass ratio binary system with about 0.2 possessing a moderate degree of contact. The long-term period investigation showed that the period of V458 Mon is increasing at , which could be the reason of mass transfer from the less massive component to more massive primary one, together with a periodic change. The oscillation in orbital period may be due to an unseen tertiary companion with the mass about . After removing these change, there is still a weak cyclic change maybe due to magnetic activity. With the increase in orbital period of binary, the separation increases and mass ratio decreases which eventually leads V458 Mon towards merger.
{"title":"A photometric study of a total-eclipse contact binary V458 Mon","authors":"Ahmed Waqas Zubairi , Zhao Ergang , Jiajia He , Fuxing Li , Liying Zhu , Azizbek Matekov","doi":"10.1016/j.newast.2024.102250","DOIUrl":"https://doi.org/10.1016/j.newast.2024.102250","url":null,"abstract":"<div><p>We present light curve solution of V458 Mon firstly by using the Wilson-Devinney code. The total eclipse and deep minima of the light curves of V458 Mon<!--> <!-->enable us to determine reliable orbital parameters of the binary system. The solution suggests that V458 Mon<!--> <!-->is a low mass ratio binary system with about 0.2 possessing a moderate degree of contact. The long-term period investigation showed that the period of V458 Mon<!--> <!-->is increasing at <span><math><mrow><mi>d</mi><mi>P</mi><mo>/</mo><mi>d</mi><mi>t</mi><mo>=</mo><mo>+</mo><mn>2</mn><mo>.</mo><mn>59</mn><mo>×</mo><mn>1</mn><msup><mrow><mn>0</mn></mrow><mrow><mo>−</mo><mn>7</mn></mrow></msup><mi>d</mi><mi>a</mi><mi>y</mi><mi>s</mi><mo>/</mo><mi>y</mi><mi>r</mi></mrow></math></span>, which could be the reason of mass transfer from the less massive component to more massive primary one, together with a periodic change. The oscillation in orbital period may be due to an unseen tertiary companion with the mass about <span><math><mrow><msub><mrow><mi>M</mi></mrow><mrow><mn>3</mn></mrow></msub><mo>=</mo><mn>1</mn><mo>.</mo><mn>8</mn><msub><mrow><mi>M</mi></mrow><mrow><mo>⊙</mo></mrow></msub></mrow></math></span> . After removing these change, there is still a weak cyclic change maybe due to magnetic activity. With the increase in orbital period of binary, the separation increases and mass ratio decreases which eventually leads V458 Mon<!--> <!-->towards merger.</p></div>","PeriodicalId":54727,"journal":{"name":"New Astronomy","volume":null,"pages":null},"PeriodicalIF":2.0,"publicationDate":"2024-05-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141097814","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 : 2024-05-14DOI: 10.1016/j.newast.2024.102251
Joginder Singh Dhiman, Mehak Mahajan
This paper studies the combined effects of radiation and galactic cosmic ray pressures on the gravitational instability of magnetized and rotating viscoelastic fluids. The dispersion relations are derived using the normal mode analysis and discussed in the hydrodynamic (weakly coupled fluid) and kinetic (strongly coupled fluid) limits. These dispersion relations are analyzed separately for transverse and longitudinal wave propagation modes. Jeans instability criteria are obtained for kinetic and hydrodynamic limits for both modes of wave propagation, and it is found that the critical Jeans wavenumbers in each case are modified due to the presence of viscoelastic effects, radiation and cosmic rays pressures, and Alfvên wave velocity. It is also observed that the radiation pressure, cosmic ray pressure and viscoelastic parameters suppress the growth rate and thus have stabilizing effects on the Jeans instability. However, cosmic ray diffusion has a destabilizing effect on the onset of gravitational instability. The effects of various parameters on the growth rate of instability are calculated numerically and the outcomes are depicted graphically. The results of the present analysis shall be helpful in understanding the impact of cosmic rays and radiative mechanisms on the gravitational collapse in the viscoelastic region of molecular cloud clumps.
{"title":"Radiation pressure and galactic cosmic rays-driven gravitational instability in rotating and magnetized viscoelastic fluids","authors":"Joginder Singh Dhiman, Mehak Mahajan","doi":"10.1016/j.newast.2024.102251","DOIUrl":"10.1016/j.newast.2024.102251","url":null,"abstract":"<div><p>This paper studies the combined effects of radiation and galactic cosmic ray pressures on the gravitational instability of magnetized and rotating viscoelastic fluids. The dispersion relations are derived using the normal mode analysis and discussed in the hydrodynamic (weakly coupled fluid) and kinetic (strongly coupled fluid) limits. These dispersion relations are analyzed separately for transverse and longitudinal wave propagation modes. Jeans instability criteria are obtained for kinetic and hydrodynamic limits for both modes of wave propagation, and it is found that the critical Jeans wavenumbers in each case are modified due to the presence of viscoelastic effects, radiation and cosmic rays pressures, and Alfvên wave velocity. It is also observed that the radiation pressure, cosmic ray pressure and viscoelastic parameters suppress the growth rate and thus have stabilizing effects on the Jeans instability. However, cosmic ray diffusion has a destabilizing effect on the onset of gravitational instability. The effects of various parameters on the growth rate of instability are calculated numerically and the outcomes are depicted graphically. The results of the present analysis shall be helpful in understanding the impact of cosmic rays and radiative mechanisms on the gravitational collapse in the viscoelastic region of molecular cloud clumps.</p></div>","PeriodicalId":54727,"journal":{"name":"New Astronomy","volume":null,"pages":null},"PeriodicalIF":2.0,"publicationDate":"2024-05-14","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141026716","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 : 2024-05-08DOI: 10.1016/j.newast.2024.102249
Akhil Uniyal , Sayan Chakrabarti , Reggie C. Pantig , Ali Övgün
In this paper, we explore the effect of the parameters of non-linear electrodynamics (NLED) and magnetic charges on various aspects of black holes (BH) arising in the particular NLED theory. More precisely, we look into the behavior of photons around the BH and produce shadow by considering a thin accretion disk model. We initially examine the overall behavior of the photon sphere and the corresponding shadow silhouette under the effects of these parameters. Using the EHT data for Sgr. A* and M87*, we provide constraints on the magnetic charge . Our results indicate that M87* gives better constraints, and as the value of the NLED coupling parameter is increased, the constrained range for widens. At lower values of , we find that the shadow radius is close to the observed value. Then, we study different other aspects, such as the energy emitted by the accretion disk, the temperature of the disk around the BH, and the nature of light it gives off. We also look at how the black hole shadow appears in different situations. Finally, we investigate how the magnetic charge affects all the above mentioned aspects when we take into account NLED along with gravity. This study helps us understand the complex relationship between magnetic charge and its effect on various aspects related to a BH.
{"title":"Nonlinearly charged black holes: Shadow and thin-accretion disk","authors":"Akhil Uniyal , Sayan Chakrabarti , Reggie C. Pantig , Ali Övgün","doi":"10.1016/j.newast.2024.102249","DOIUrl":"https://doi.org/10.1016/j.newast.2024.102249","url":null,"abstract":"<div><p>In this paper, we explore the effect of the parameters of non-linear electrodynamics (NLED) and magnetic charges on various aspects of black holes (BH) arising in the particular NLED theory. More precisely, we look into the behavior of photons around the BH and produce shadow by considering a thin accretion disk model. We initially examine the overall behavior of the photon sphere and the corresponding shadow silhouette under the effects of these parameters. Using the EHT data for Sgr. A* and M87*, we provide constraints on the magnetic charge <span><math><msub><mrow><mi>q</mi></mrow><mrow><mi>m</mi></mrow></msub></math></span>. Our results indicate that M87* gives better constraints, and as the value of the NLED coupling parameter <span><math><mi>β</mi></math></span> is increased, the constrained range for <span><math><msub><mrow><mi>q</mi></mrow><mrow><mi>m</mi></mrow></msub></math></span> widens. At lower values of <span><math><msub><mrow><mi>q</mi></mrow><mrow><mi>m</mi></mrow></msub></math></span>, we find that the shadow radius is close to the observed value. Then, we study different other aspects, such as the energy emitted by the accretion disk, the temperature of the disk around the BH, and the nature of light it gives off. We also look at how the black hole shadow appears in different situations. Finally, we investigate how the magnetic charge affects all the above mentioned aspects when we take into account NLED along with gravity. This study helps us understand the complex relationship between magnetic charge and its effect on various aspects related to a BH.</p></div>","PeriodicalId":54727,"journal":{"name":"New Astronomy","volume":null,"pages":null},"PeriodicalIF":2.0,"publicationDate":"2024-05-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140909802","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}
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":null,"pages":null},"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":null,"pages":null},"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":null,"pages":null},"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
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 =0.9026. 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 Dor pulsator in the main-sequence stage with a rotation period of about 5.7 days, rotating slower than the orbital motion. The fundamental parameters of two components are firstly estimated as follows: =1.53 M , = 1.38 M , =7240 K, =6747 K, =1.8288 R , = 1.3075 R ,
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":null,"pages":null},"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":null,"pages":null},"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
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 = 1.47 and with an age of Gyr for HD 80671, and and with an age of Gyr for HD 97038. The improved dynamical parallaxes are given as mas for HD 80671, and 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":null,"pages":null},"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}