Pub Date : 2024-07-27DOI: 10.1016/j.newast.2024.102290
Yun-A Jo, Heon-Young Chang
In this study, we have explored the frequency separations, and , the height and width of the oscillation power excess, and , as a function of the frequency of maximum power by analyzing 187 evolved stars in six star clusters observed by the Kepler/K2 missions. We have also examined the asteroseismic relation in the Christensen-Dalsgaard diagram. Given the importance of scaling relations, the dependency of asteroseismic scaling relations on physical quantities must be verified to reduce systematic errors through the exploration of observational data obtained from various sources. In this context, the star cluster provides a valuable means to assess the age and metallicity. Focusing on evolved stars with , we have exploited the mass effect without the need for deriving the individual stellar mass. We have found that the considered relations appear to be associated with the age of star clusters, thereby the mass of the stars in a given evolutionary status for star clusters with different ages. By separately considering red giant branch stars and red clump stars, we have found that red clump stars appear more sensitive to the cluster age compared with red giant branch stars. It has been suggested that conclusions regarding the dependency of metallicity should be drawn with due care as outcomes are subject to how to treat metallicity. Finally, we conclude by briefly pointing out implications of our findings on asteroseismic inferences.
{"title":"Asteroseismology of evolved stars in six star clusters observed by Kepler/K2","authors":"Yun-A Jo, Heon-Young Chang","doi":"10.1016/j.newast.2024.102290","DOIUrl":"10.1016/j.newast.2024.102290","url":null,"abstract":"<div><p>In this study, we have explored the frequency separations, <span><math><mrow><mi>Δ</mi><mi>ν</mi></mrow></math></span> and <span><math><mrow><mi>δ</mi><msub><mrow><mi>ν</mi></mrow><mrow><mn>02</mn></mrow></msub></mrow></math></span>, the height and width of the oscillation power excess, <span><math><msub><mrow><mi>H</mi></mrow><mrow><mi>Gauss</mi></mrow></msub></math></span> and <span><math><mrow><mi>δ</mi><msub><mrow><mi>ν</mi></mrow><mrow><mi>env</mi></mrow></msub></mrow></math></span>, as a function of the frequency of maximum power <span><math><msub><mrow><mi>ν</mi></mrow><mrow><mi>max</mi></mrow></msub></math></span> by analyzing 187 evolved stars in six star clusters observed by the <em>Kepler</em>/<em>K2</em> missions. We have also examined the asteroseismic relation in the Christensen-Dalsgaard diagram. Given the importance of scaling relations, the dependency of asteroseismic scaling relations on physical quantities must be verified to reduce systematic errors through the exploration of observational data obtained from various sources. In this context, the star cluster provides a valuable means to assess the age and metallicity. Focusing on evolved stars with <span><math><mrow><mn>30</mn><mspace></mspace><mi>μ</mi><mi>Hz</mi><mo><</mo><msub><mrow><mi>ν</mi></mrow><mrow><mi>max</mi></mrow></msub><mo><</mo><mn>220</mn><mspace></mspace><mi>μ</mi><mi>Hz</mi></mrow></math></span>, we have exploited the mass effect without the need for deriving the individual stellar mass. We have found that the considered relations appear to be associated with the age of star clusters, thereby the mass of the stars in a given evolutionary status for star clusters with different ages. By separately considering red giant branch stars and red clump stars, we have found that red clump stars appear more sensitive to the cluster age compared with red giant branch stars. It has been suggested that conclusions regarding the dependency of metallicity should be drawn with due care as outcomes are subject to how to treat metallicity. Finally, we conclude by briefly pointing out implications of our findings on asteroseismic inferences.</p></div>","PeriodicalId":54727,"journal":{"name":"New Astronomy","volume":"113 ","pages":"Article 102290"},"PeriodicalIF":1.9,"publicationDate":"2024-07-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141849232","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 : 2024-07-27DOI: 10.1016/j.newast.2024.102289
J.M. Ohlert , A. Richichi
Following up on our initial paper (Richichi and Ohlert, 2021), we report here on 60 lunar occultation events recorded between February 2021 and March 2024 at the Michael Adrian Observatorium. An improved version of the detector was employed for the present work. The program aims mainly at the direct measurement of the angular diameter of late-type stars, and the discovery or confirmation of binary stars with small separations. Among the results, we present first time angular diameter determinations for the late-type M giants IRC +20184 and BL Tau and for the bright carbon star TU Gem. Our diameter result for RX Cnc is the first determination outside the near-IR range. We also discovered or detected directly for the first time companions around SAO 79580, BL Tau again, and SAO 78643. The lunar occultation technique at our facility is capable to reach sources as faint as 10 V magnitude with an angular resolution at the milliarcsecond level.
{"title":"Further lunar occultations results from the Trebur Observatory, 2021–24","authors":"J.M. Ohlert , A. Richichi","doi":"10.1016/j.newast.2024.102289","DOIUrl":"10.1016/j.newast.2024.102289","url":null,"abstract":"<div><p>Following up on our initial paper (Richichi and Ohlert, 2021), we report here on 60 lunar occultation events recorded between February 2021 and March 2024 at the Michael Adrian Observatorium. An improved version of the detector was employed for the present work. The program aims mainly at the direct measurement of the angular diameter of late-type stars, and the discovery or confirmation of binary stars with small separations. Among the results, we present first time angular diameter determinations for the late-type M giants IRC +20184 and BL Tau and for the bright carbon star TU Gem. Our diameter result for RX Cnc is the first determination outside the near-IR range. We also discovered or detected directly for the first time companions around SAO 79580, BL Tau again, and SAO 78643. The lunar occultation technique at our facility is capable to reach sources as faint as <span><math><mo>≈</mo></math></span> 10<!--> <!-->V magnitude with an angular resolution at the milliarcsecond level.</p></div>","PeriodicalId":54727,"journal":{"name":"New Astronomy","volume":"113 ","pages":"Article 102289"},"PeriodicalIF":1.9,"publicationDate":"2024-07-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S1384107624001039/pdfft?md5=87c54c6a624308f0bc6941d3934cc2c9&pid=1-s2.0-S1384107624001039-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141845323","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}
In this article, we study solutions which describe wormholes in the halos of dwarf and massive spiral galaxies with different morphologies, masses, sizes and gas fractions by taking observed flat rotation curves as input. We assume Singular Isothermal Sphere (SIS) dark matter density profile. This result confirms the possible existence of wormholes in both dwarf and massive spiral galaxies.
{"title":"Wormholes in dwarf and spiral galactic halo regions","authors":"Mehedi Kalam , Amir Ghari , Irina Radinschi , Hosein Haghi , Farook Rahaman , Tandrima Chowdhury","doi":"10.1016/j.newast.2024.102288","DOIUrl":"10.1016/j.newast.2024.102288","url":null,"abstract":"<div><p>In this article, we study solutions which describe wormholes in the halos of dwarf and massive spiral galaxies with different morphologies, masses, sizes and gas fractions by taking observed flat rotation curves as input. We assume Singular Isothermal Sphere (SIS) dark matter density profile. This result confirms the possible existence of wormholes in both dwarf and massive spiral galaxies.</p></div>","PeriodicalId":54727,"journal":{"name":"New Astronomy","volume":"113 ","pages":"Article 102288"},"PeriodicalIF":1.9,"publicationDate":"2024-07-20","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141852015","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 : 2024-07-15DOI: 10.1016/j.newast.2024.102287
Gabriela de Carvalho Assis Goulart , Thiago Statella , Rafael Sfair
In 2012, Brazil began the studies to send its first deep space exploration mission, ASTER, which would be the first mission to orbit a triple asteroid system, 2001 SN263. We aim to contribute to the ASTER mission by defining the parameters of a multispectral camera system that will be used to study the asteroid system 2001 SN263, through software simulations that should help planning the data collection. We inserted the shape model of the objects in the software POV-Ray and modeled two cameras, a Wide Angle (WAC) and a Narrow Angle (NAC). We inserted the asteroid's parameters and simulated the satellite position. We created various scenes so we could obtain a good view of the asteroid. Alpha is entirely visible only in the WAC images, while the NAC is expected to reveal surface details. Beta seems relatively small in the WAC images, whereas we obtain a broad view from the NAC at 100 km distance. Gamma, smaller than Beta, should provide more detailed images through the NAC, whereas the WAC images should be able to show its inclined orbit around Alpha. To see Gamma behind Alpha in its revolution movement, we would have to elevate the camera's orbit. The method employed to simulate images generated by satellite cameras can be applied to other scenarios where the target requires imaging, extending beyond the field of planetary geology.
{"title":"Definition of multispectral camera system parameters to model the asteroid 2001 SN263","authors":"Gabriela de Carvalho Assis Goulart , Thiago Statella , Rafael Sfair","doi":"10.1016/j.newast.2024.102287","DOIUrl":"10.1016/j.newast.2024.102287","url":null,"abstract":"<div><p>In 2012, Brazil began the studies to send its first deep space exploration mission, ASTER, which would be the first mission to orbit a triple asteroid system, 2001 SN263. We aim to contribute to the ASTER mission by defining the parameters of a multispectral camera system that will be used to study the asteroid system 2001 SN263, through software simulations that should help planning the data collection. We inserted the shape model of the objects in the software POV-Ray and modeled two cameras, a Wide Angle (WAC) and a Narrow Angle (NAC). We inserted the asteroid's parameters and simulated the satellite position. We created various scenes so we could obtain a good view of the asteroid. Alpha is entirely visible only in the WAC images, while the NAC is expected to reveal surface details. Beta seems relatively small in the WAC images, whereas we obtain a broad view from the NAC at 100 km distance. Gamma, smaller than Beta, should provide more detailed images through the NAC, whereas the WAC images should be able to show its inclined orbit around Alpha. To see Gamma behind Alpha in its revolution movement, we would have to elevate the camera's orbit. The method employed to simulate images generated by satellite cameras can be applied to other scenarios where the target requires imaging, extending beyond the field of planetary geology.</p></div>","PeriodicalId":54727,"journal":{"name":"New Astronomy","volume":"113 ","pages":"Article 102287"},"PeriodicalIF":1.9,"publicationDate":"2024-07-15","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141712259","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 this paper, we study the curved Krori–Barua spacetime geometry to describe compact stars with two components: dark and ordinary matter, using a two-fluid model approach. We choose the equation of state derived from the rotational curves of galaxies for dark matter and the polytropic equation of state for ordinary matter. The physical requirements for a realistic compact star are satisfied using specific parameters. For the polytropic index , we find the values of observed masses, reported in our previous investigation (Mafa et al., 2020).
{"title":"Modeling compact stars with two fluids","authors":"Pedro Mafa , Vishnu Kakkat , Amos Kubeka , Mantile Lekala","doi":"10.1016/j.newast.2024.102286","DOIUrl":"10.1016/j.newast.2024.102286","url":null,"abstract":"<div><p>In this paper, we study the curved Krori–Barua spacetime geometry to describe compact stars with two components: dark and ordinary matter, using a two-fluid model approach. We choose the equation of state derived from the rotational curves of galaxies for dark matter and the polytropic equation of state for ordinary matter. The physical requirements for a realistic compact star are satisfied using specific parameters. For the polytropic index <span><math><mrow><mi>η</mi><mo>=</mo><mn>2</mn></mrow></math></span>, we find the values of observed masses, reported in our previous investigation (Mafa et al., 2020).</p></div>","PeriodicalId":54727,"journal":{"name":"New Astronomy","volume":"113 ","pages":"Article 102286"},"PeriodicalIF":1.9,"publicationDate":"2024-07-11","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S1384107624001003/pdfft?md5=051c3f9eade0b3342ac0112088c30b75&pid=1-s2.0-S1384107624001003-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141637662","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}
Pub Date : 2024-07-11DOI: 10.1016/j.newast.2024.102276
Maryam Ghasemnezhad , Mohsen Khosravi
Recent observational evidence confirms the weak-collision dynamics of hot optically thin accretion flows around Sgr A and other nearby galactic nuclei. As a result, thermal conduction as a diffusion process can transfer the heat by electrons in a collisionless magnetized plasma. While most of the previous analytical studies consider the azimuthal viscosity, the recent studies indicated that the radial viscosity strongly affects the properties of the advection dominated accretion discs. So, in this paper, we explore the roles of two parts of anisotropic thermal conduction (parallel and perpendicular) and radial viscosity in the hot accretion disc by considering axisymmetric and steady state assumptions in the presence of outflows that can transport energy from accretion disc outward. We use the set of self-similar solutions to solve the basic equations in our present model. Our solutions reveal that transverse thermal conduction as a cooling mechanism, leads to reductions in gas temperature, disc thickness, and accretion velocity of the disc, whereas the disc rotates at a fast rate. Moreover Our solutions indicate that the perpendicular thermal conduction and the radial viscosity have opposite behavior in the physical variables of the disc. Also, our results have indicated that the anisotropic thermal conduction is significant in the parameter space of radial viscosity, outflow in the regions that the physical constraints and are satisfied.
{"title":"The role of radial viscosity force and anisotropic thermal conduction in hot accretion flow","authors":"Maryam Ghasemnezhad , Mohsen Khosravi","doi":"10.1016/j.newast.2024.102276","DOIUrl":"10.1016/j.newast.2024.102276","url":null,"abstract":"<div><p>Recent observational evidence confirms the weak-collision dynamics of hot optically thin accretion flows around Sgr A<span><math><msup><mrow></mrow><mrow><mo>∗</mo></mrow></msup></math></span> and other nearby galactic nuclei. As a result, thermal conduction as a diffusion process can transfer the heat by electrons in a collisionless magnetized plasma. While most of the previous analytical studies consider the azimuthal viscosity, the recent studies indicated that the radial viscosity strongly affects the properties of the advection dominated accretion discs. So, in this paper, we explore the roles of two parts of anisotropic thermal conduction (parallel and perpendicular) and radial viscosity in the hot accretion disc by considering axisymmetric and steady state assumptions in the presence of outflows that can transport energy from accretion disc outward. We use the set of self-similar solutions to solve the basic equations in our present model. Our solutions reveal that transverse thermal conduction as a cooling mechanism, leads to reductions in gas temperature, disc thickness, and accretion velocity of the disc, whereas the disc rotates at a fast rate. Moreover Our solutions indicate that the perpendicular thermal conduction and the radial viscosity have opposite behavior in the physical variables of the disc. Also, our results have indicated that the anisotropic thermal conduction is significant in the parameter space of radial viscosity, outflow in the regions that the physical constraints <span><math><mrow><msub><mrow><mi>t</mi></mrow><mrow><mi>i</mi><mi>n</mi></mrow></msub><mo>≥</mo><msub><mrow><mi>t</mi></mrow><mrow><mo>⊥</mo><mo>,</mo><mi>c</mi><mi>o</mi><mi>n</mi></mrow></msub></mrow></math></span> and <span><math><mrow><msub><mrow><mi>q</mi></mrow><mrow><mo>∥</mo><mo>,</mo><mi>c</mi><mi>o</mi><mi>n</mi></mrow></msub><mo>⩽</mo><msub><mrow><mi>q</mi></mrow><mrow><mo>⊥</mo><mo>,</mo><mi>c</mi><mi>o</mi><mi>n</mi></mrow></msub></mrow></math></span> are satisfied.</p></div>","PeriodicalId":54727,"journal":{"name":"New Astronomy","volume":"113 ","pages":"Article 102276"},"PeriodicalIF":1.9,"publicationDate":"2024-07-11","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141696176","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 : 2024-07-06DOI: 10.1016/j.newast.2024.102273
G.M. Hamed , H.H. Esenoglu , A.I. Galeev
We present spectroscopic observations of Nova Cas 2020 (V1391 Cas) obtained using the Russian Turkish Telescope during different stages of its 2020 outburst. We followed the spectral evolution of the nova until it entered the nebular phase. The expansion velocity of the ejecta reached . The fluxes of the neutral [O I] lines at wavelengths 6300, 6364, and 5577 were used to calculate the electron temperature and the mass of neutral oxygen in the ejecta. We found average values , which are consistent with the values calculated for other novae. We modeled the nova’s ejected envelope 515 days after its discovery and found that the log elemental abundances by number relative to Hydrogen of the envelope are He = −0.7, C = −5.5, O = −2.5, N = −2.0 and Ne = −4.0.
我们介绍了利用俄罗斯土耳其望远镜在新星 Cas 2020(V1391 Cas)爆发的不同阶段对其进行的光谱观测。我们跟踪了新星的光谱演变过程,直到它进入星云阶段。喷出物的膨胀速度达到了 ∼780km s-1。我们利用波长为6300、6364和5577̊A的中性[O I]线的通量来计算喷出物中的电子温度和中性氧的质量。我们发现Te=4890K,MOI=2.54×10-5M⊙的平均值与其他新星的计算值一致。我们在发现新星515天后对其喷出包层进行了建模,发现包层中相对于氢的对数元素丰度为He=-0.7、C=-5.5、O=-2.5、N=-2.0和Ne=-4.0。
{"title":"Spectral evolution and photo-ionization analysis of Nova Cas 2020 (V1391 Cas)","authors":"G.M. Hamed , H.H. Esenoglu , A.I. Galeev","doi":"10.1016/j.newast.2024.102273","DOIUrl":"https://doi.org/10.1016/j.newast.2024.102273","url":null,"abstract":"<div><p>We present spectroscopic observations of Nova Cas 2020 <strong>(V1391 Cas)</strong> obtained using the Russian Turkish Telescope during different stages of its 2020 outburst. We followed the spectral evolution of the nova until it entered the nebular phase. The expansion velocity of the ejecta reached <span><math><mrow><mo>∼</mo><mn>780</mn><mspace></mspace><msup><mrow><mi>km s</mi></mrow><mrow><mo>−</mo><mn>1</mn></mrow></msup></mrow></math></span>. The fluxes of the neutral [O I] lines at wavelengths 6300, 6364, and 5577 <span><math><mtext>̊A</mtext></math></span> were used to calculate the electron temperature and the mass of neutral oxygen in the ejecta. We found average values <span><math><mrow><msub><mrow><mi>T</mi></mrow><mrow><mi>e</mi></mrow></msub><mo>=</mo><mi>4890</mi><mspace></mspace><mi>K</mi></mrow></math></span>, <span><math><mrow><msub><mrow><mi>M</mi></mrow><mrow><mi>OI</mi></mrow></msub><mo>=</mo><mi>2.54</mi><mo>×</mo><msup><mrow><mi>10</mi></mrow><mrow><mi>−5</mi></mrow></msup><msub><mrow><mi>M</mi></mrow><mrow><mo>⊙</mo></mrow></msub></mrow></math></span> which are consistent with the values calculated for other novae. We modeled the nova’s ejected envelope 515 days after its discovery and found that the log elemental abundances by number relative to Hydrogen of the envelope are He = −0.7, C = −5.5, O = −2.5, N = −2.0 and Ne = −4.0.</p></div>","PeriodicalId":54727,"journal":{"name":"New Astronomy","volume":"113 ","pages":"Article 102273"},"PeriodicalIF":1.9,"publicationDate":"2024-07-06","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141605542","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 : 2024-07-04DOI: 10.1016/j.newast.2024.102274
Syed Mudassir Syed Iqbal , G.U. Khapekar , S.H. Shekh , A. Dixit
we explored the holographic dark energy model using Hubble’s Horizon as the infrared (IR) cut-off in Locally Rotationally Symmetric (LRS) Bianchi type-I, considering the gravity framework in our analysis. In order to solve the field equations, we assume a relation and volumetric power law expansion (where is constant). we have expressed various crucial cosmological parameters in terms of the redshift and depicted them graphically to enhance our understanding of the expansion and evolution of the universe like holographic dark energy density (), holographic dark energy pressure (), equation of state parameter () , total energy density parameter () etc. Also, we analyzed the stability of the universe in our model through the squared speed of sound test and its validity by energy conditions. Ultimately, our model indicates that the universe is currently in an expanding phase, exhibiting an accelerating phase, closely approaching a flat geometry, and its behavior resembles that of a quintessence dark energy model.
我们探索了全息暗能量模型,将哈勃地平线(Hubble's Horizon)作为局部旋转对称(LRS)边奇 I 型的红外(IR)截止点,并在分析中考虑了引力框架。为了求解场方程,我们假设了一个关系和体积幂律膨胀(其中为常数)。我们用红移表示了各种关键的宇宙学参数,并用图形描述了它们,以加深我们对宇宙膨胀和演化的理解,如全息暗能量密度()、全息暗能量压力()、状态方程参数()、总能量密度参数()等。此外,我们还通过声速平方检验分析了我们模型中宇宙的稳定性及其在能量条件下的有效性。最终,我们的模型表明,宇宙目前正处于膨胀阶段,表现出加速阶段,接近于平面几何,其行为类似于五元暗能量模型。
{"title":"LRS Bianchi type-I with Hubble’s horizon as IR cut-off in f(R) gravity","authors":"Syed Mudassir Syed Iqbal , G.U. Khapekar , S.H. Shekh , A. Dixit","doi":"10.1016/j.newast.2024.102274","DOIUrl":"10.1016/j.newast.2024.102274","url":null,"abstract":"<div><p>we explored the holographic dark energy model using Hubble’s Horizon as the infrared (IR) cut-off in Locally Rotationally Symmetric (LRS) Bianchi type-I, considering the <span><math><mrow><mi>f</mi><mrow><mo>(</mo><mi>R</mi><mo>)</mo></mrow></mrow></math></span> gravity framework in our analysis. In order to solve the field equations, we assume a relation <span><math><mrow><mi>F</mi><mo>∝</mo><mspace></mspace><msup><mrow><mi>a</mi></mrow><mrow><mi>m</mi></mrow></msup></mrow></math></span> and volumetric power law expansion (where <span><math><mi>m</mi></math></span> is constant). we have expressed various crucial cosmological parameters in terms of the redshift <span><math><mi>z</mi></math></span> and depicted them graphically to enhance our understanding of the expansion and evolution of the universe like holographic dark energy density (<span><math><msub><mrow><mi>ρ</mi></mrow><mrow><mi>Λ</mi></mrow></msub></math></span>), holographic dark energy pressure (<span><math><msub><mrow><mi>p</mi></mrow><mrow><mi>Λ</mi></mrow></msub></math></span>), equation of state parameter (<span><math><mi>ω</mi></math></span>) , total energy density parameter (<span><math><mi>Ω</mi></math></span>) etc. Also, we analyzed the stability of the universe in our model through the squared speed of sound test and its validity by energy conditions. Ultimately, our model indicates that the universe is currently in an expanding phase, exhibiting an accelerating phase, closely approaching a flat geometry, and its behavior resembles that of a quintessence dark energy model.</p></div>","PeriodicalId":54727,"journal":{"name":"New Astronomy","volume":"113 ","pages":"Article 102274"},"PeriodicalIF":1.9,"publicationDate":"2024-07-04","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141587749","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 : 2024-07-02DOI: 10.1016/j.newast.2024.102275
Eugene Oks
In attempts to resolve the neutron lifetime puzzle, there was suggested a hypothetical decay of neutrons into some unspecified dark matter (DM) particles. Later there were performed studies on how the hypothetical decay of neutrons would affect neutron stars. Recently it was shown that with the allowance for the second solution of Dirac equation for hydrogen atoms, the theoretical branching ratio (BR) for the two-body decay of neutrons (compared to their three-body decay) is amplified by a factor of 3300 from 0.000004. So, the BR becomes about 1.3% in the excellent agreement with the “experimental” BR = (1.15 ± 0.27)% required for reconciling the two distinct experimental values of the neutron lifetime: one from the beam experiments, another from the trap experiments. This meant that the two-body decay of neutrons in the beam experiments (that count only the protons) plays a much more sizable part in the overestimation of the lifetime of neutrons in these experiments than previously thought. Hydrogen atoms corresponding to the second solution of Dirac equations are called the second flavor of hydrogen atoms (SFHA) by the analogy with the flavors of quarks. The existence of the SFHA is evidenced by four different types of atomic/molecular experiments. The primary feature of the SFHA is that due to having only the s-states, they do not emit or absorb the electromagnetic radiation (except for the 21 cm line): they are practically dark. The SFHA became a candidate for a part of DM for the first time after the SFHA-based successful qualitative and quantitative explanation of the perplexing observation by Bowman et al. of the anomalous absorption in the redshifted 21 cm line from the early Universe. In the present paper we analyzed how this neutron decay into the SFHA affects neutron stars. We showed that old neutron stars could very slowly generate the new specific, described in detail baryonic DM in the form of the SFHA. Some old neutron stars would release it into their tiny atmospheres, while some other old neutron stars would release it into the interstellar medium. Besides, mergers of a neutron star with another neutron star or with a black hole, accompanied by the ejection of neutron-rich material, can also lead to the formation of SFHA as the ejecta cools down. This is another interesting aspect of the multi-messenger astronomy focused on studying these mergers through the gravitational waves they generate. These mechanisms of generating new baryonic DM in the universe should have the fundamental importance. We point out the indirect observational evidence of the continuing generation of new baryonic DM. We hope that our results will stimulate a further research in this direction.
{"title":"New results on the two-body decay of neutrons shed new light on neutron stars","authors":"Eugene Oks","doi":"10.1016/j.newast.2024.102275","DOIUrl":"10.1016/j.newast.2024.102275","url":null,"abstract":"<div><p>In attempts to resolve the neutron lifetime puzzle, there was suggested a hypothetical decay of neutrons into some <em>unspecified</em> dark matter (DM) particles. Later there were performed studies on how the hypothetical decay of neutrons would affect neutron stars. Recently it was shown that with the allowance for the second solution of Dirac equation for hydrogen atoms, the theoretical branching ratio (BR) for the two-body decay of neutrons (compared to their three-body decay) is amplified by a factor of 3300 from 0.000004. So, the BR becomes about 1.3% in the excellent agreement with the “experimental” BR = (1.15 ± 0.27)% required for reconciling the two distinct experimental values of the neutron lifetime: one from the beam experiments, another from the trap experiments. This meant that the two-body decay of neutrons in the beam experiments (that count only the protons) plays a much more sizable part in the overestimation of the lifetime of neutrons in these experiments than previously thought. Hydrogen atoms corresponding to the second solution of Dirac equations are called the second flavor of hydrogen atoms (SFHA) by the analogy with the flavors of quarks. The existence of the SFHA is evidenced by four different types of atomic/molecular experiments. The primary feature of the SFHA is that due to having only the s-states, they do not emit or absorb the electromagnetic radiation (except for the 21 cm line): they are practically <em>dark</em>. The SFHA became a candidate for a part of DM for the first time after the SFHA-based successful qualitative and quantitative explanation of the perplexing observation by Bowman et al. of the anomalous absorption in the redshifted 21 cm line from the early Universe. In the present paper we analyzed how this neutron decay into the SFHA affects neutron stars. We showed that old neutron stars could very slowly generate the new <em>specific, described in detail</em> baryonic DM in the form of the SFHA. Some old neutron stars would release it into their tiny atmospheres, while some other old neutron stars would release it into the interstellar medium. Besides, mergers of a neutron star with another neutron star or with a black hole, accompanied by the ejection of neutron-rich material, can also lead to the formation of SFHA as the ejecta cools down. This is another interesting aspect of the multi-messenger astronomy focused on studying these mergers through the gravitational waves they generate. These mechanisms of generating new baryonic DM in the universe should have the fundamental importance. We point out the indirect observational evidence of the continuing generation of new baryonic DM. We hope that our results will stimulate a further research in this direction.</p></div>","PeriodicalId":54727,"journal":{"name":"New Astronomy","volume":"113 ","pages":"Article 102275"},"PeriodicalIF":1.9,"publicationDate":"2024-07-02","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141587750","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 : 2024-06-30DOI: 10.1016/j.newast.2024.102272
Absos Ali Shaikh , Faizuddin Ahmed , Mousumi Sarkar
<div><p>The objective of this article is to study topologically charged Eddington-inspired Born–Infeld (briefly, EiBI) gravity spacetime. It is proved that the topologically charged EiBI spacetime executes different types of pseudosymmetry, viz. Ricci generalized pseudosymmetry as <span><math><mrow><mi>R</mi><mi>⋅</mi><mi>R</mi><mo>=</mo><mi>Q</mi><mrow><mo>(</mo><mi>S</mi><mo>,</mo><mi>R</mi><mo>)</mo></mrow></mrow></math></span>, Ricci generalized projectively pseudosymmetry as <span><math><mrow><mi>P</mi><mi>⋅</mi><mi>R</mi><mo>=</mo><mfrac><mrow><mn>2</mn></mrow><mrow><mn>3</mn></mrow></mfrac><mi>Q</mi><mrow><mo>(</mo><mi>S</mi><mo>,</mo><mi>R</mi><mo>)</mo></mrow></mrow></math></span>, pseudosymmetry due to conformal curvature as <span><math><mrow><mi>C</mi><mi>⋅</mi><mi>C</mi><mo>=</mo><mo>−</mo><mfrac><mrow><mrow><mo>(</mo><msup><mrow><mi>r</mi></mrow><mrow><mn>2</mn></mrow></msup><msup><mrow><mi>α</mi></mrow><mrow><mn>2</mn></mrow></msup><mo>+</mo><mn>2</mn><mi>ϵ</mi><msup><mrow><mi>α</mi></mrow><mrow><mn>2</mn></mrow></msup><mo>−</mo><msup><mrow><mi>r</mi></mrow><mrow><mn>2</mn></mrow></msup><mo>)</mo></mrow></mrow><mrow><mn>6</mn><msup><mrow><mi>r</mi></mrow><mrow><mn>4</mn></mrow></msup></mrow></mfrac><mi>Q</mi><mrow><mo>(</mo><mi>g</mi><mo>,</mo><mi>C</mi><mo>)</mo></mrow></mrow></math></span> and pseudosymmetry due to conharmonic curvature as <span><math><mrow><mi>K</mi><mi>⋅</mi><mi>K</mi><mo>=</mo><mo>−</mo><mfrac><mrow><mrow><mo>(</mo><msup><mrow><mi>α</mi></mrow><mrow><mn>2</mn></mrow></msup><mo>−</mo><mn>1</mn><mo>)</mo></mrow></mrow><mrow><mn>2</mn><msup><mrow><mi>r</mi></mrow><mrow><mn>2</mn></mrow></msup></mrow></mfrac><mi>Q</mi><mrow><mo>(</mo><mi>g</mi><mo>,</mo><mi>K</mi><mo>)</mo></mrow></mrow></math></span>. Also, we have exhibited the linear dependence of <span><math><mrow><mi>Q</mi><mrow><mo>(</mo><mi>g</mi><mo>,</mo><mi>C</mi><mo>)</mo></mrow></mrow></math></span> and <span><math><mrow><mi>Q</mi><mrow><mo>(</mo><mi>S</mi><mo>,</mo><mi>C</mi><mo>)</mo></mrow></mrow></math></span> on the difference <span><math><mrow><mo>(</mo><mi>C</mi><mi>⋅</mi><mi>R</mi><mo>−</mo><mi>R</mi><mi>⋅</mi><mi>C</mi><mo>)</mo></mrow></math></span>. Moreover, it is exhibited that the topologically charged EiBI spacetime is an Einstein manifold of level 3, 2-quasi Einstein, conformal 2-forms are recurrent, Ricci 1-forms are recurrent and generalized Roter type. As a special case, we have acquired the geometric structures of point-like global monopole (briefly, PGM) spacetime and topologically charged Ellis Bronnikov Wormhole (briefly, TCEBW) spacetime. Also, we have explored that the topologically charged EiBI spacetime possesses almost <span><math><mi>η</mi></math></span>-Ricci-Yamabe soliton, almost <span><math><mi>η</mi></math></span>-Ricci soliton, and for a certain condition it admits almost Ricci soliton. Further, it is also verified that such a spacetime reveals generalized curvature inheritance and for a particular condition it admits
{"title":"Curvature related geometrical properties of topologically charged EiBI-gravity spacetime","authors":"Absos Ali Shaikh , Faizuddin Ahmed , Mousumi Sarkar","doi":"10.1016/j.newast.2024.102272","DOIUrl":"10.1016/j.newast.2024.102272","url":null,"abstract":"<div><p>The objective of this article is to study topologically charged Eddington-inspired Born–Infeld (briefly, EiBI) gravity spacetime. It is proved that the topologically charged EiBI spacetime executes different types of pseudosymmetry, viz. Ricci generalized pseudosymmetry as <span><math><mrow><mi>R</mi><mi>⋅</mi><mi>R</mi><mo>=</mo><mi>Q</mi><mrow><mo>(</mo><mi>S</mi><mo>,</mo><mi>R</mi><mo>)</mo></mrow></mrow></math></span>, Ricci generalized projectively pseudosymmetry as <span><math><mrow><mi>P</mi><mi>⋅</mi><mi>R</mi><mo>=</mo><mfrac><mrow><mn>2</mn></mrow><mrow><mn>3</mn></mrow></mfrac><mi>Q</mi><mrow><mo>(</mo><mi>S</mi><mo>,</mo><mi>R</mi><mo>)</mo></mrow></mrow></math></span>, pseudosymmetry due to conformal curvature as <span><math><mrow><mi>C</mi><mi>⋅</mi><mi>C</mi><mo>=</mo><mo>−</mo><mfrac><mrow><mrow><mo>(</mo><msup><mrow><mi>r</mi></mrow><mrow><mn>2</mn></mrow></msup><msup><mrow><mi>α</mi></mrow><mrow><mn>2</mn></mrow></msup><mo>+</mo><mn>2</mn><mi>ϵ</mi><msup><mrow><mi>α</mi></mrow><mrow><mn>2</mn></mrow></msup><mo>−</mo><msup><mrow><mi>r</mi></mrow><mrow><mn>2</mn></mrow></msup><mo>)</mo></mrow></mrow><mrow><mn>6</mn><msup><mrow><mi>r</mi></mrow><mrow><mn>4</mn></mrow></msup></mrow></mfrac><mi>Q</mi><mrow><mo>(</mo><mi>g</mi><mo>,</mo><mi>C</mi><mo>)</mo></mrow></mrow></math></span> and pseudosymmetry due to conharmonic curvature as <span><math><mrow><mi>K</mi><mi>⋅</mi><mi>K</mi><mo>=</mo><mo>−</mo><mfrac><mrow><mrow><mo>(</mo><msup><mrow><mi>α</mi></mrow><mrow><mn>2</mn></mrow></msup><mo>−</mo><mn>1</mn><mo>)</mo></mrow></mrow><mrow><mn>2</mn><msup><mrow><mi>r</mi></mrow><mrow><mn>2</mn></mrow></msup></mrow></mfrac><mi>Q</mi><mrow><mo>(</mo><mi>g</mi><mo>,</mo><mi>K</mi><mo>)</mo></mrow></mrow></math></span>. Also, we have exhibited the linear dependence of <span><math><mrow><mi>Q</mi><mrow><mo>(</mo><mi>g</mi><mo>,</mo><mi>C</mi><mo>)</mo></mrow></mrow></math></span> and <span><math><mrow><mi>Q</mi><mrow><mo>(</mo><mi>S</mi><mo>,</mo><mi>C</mi><mo>)</mo></mrow></mrow></math></span> on the difference <span><math><mrow><mo>(</mo><mi>C</mi><mi>⋅</mi><mi>R</mi><mo>−</mo><mi>R</mi><mi>⋅</mi><mi>C</mi><mo>)</mo></mrow></math></span>. Moreover, it is exhibited that the topologically charged EiBI spacetime is an Einstein manifold of level 3, 2-quasi Einstein, conformal 2-forms are recurrent, Ricci 1-forms are recurrent and generalized Roter type. As a special case, we have acquired the geometric structures of point-like global monopole (briefly, PGM) spacetime and topologically charged Ellis Bronnikov Wormhole (briefly, TCEBW) spacetime. Also, we have explored that the topologically charged EiBI spacetime possesses almost <span><math><mi>η</mi></math></span>-Ricci-Yamabe soliton, almost <span><math><mi>η</mi></math></span>-Ricci soliton, and for a certain condition it admits almost Ricci soliton. Further, it is also verified that such a spacetime reveals generalized curvature inheritance and for a particular condition it admits ","PeriodicalId":54727,"journal":{"name":"New Astronomy","volume":"112 ","pages":"Article 102272"},"PeriodicalIF":1.9,"publicationDate":"2024-06-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141587603","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}