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Temporal variability in transmission spectra of H2-dominated exoplanets: The influence of thermal evolution and stellar irradiation on atmospheric composition 以 H2 为主的系外行星透射光谱的时间变化:热演化和恒星辐照对大气成分的影响
IF 1.9 4区 物理与天体物理
New Astronomy Pub Date : 2024-08-21 DOI: 10.1016/j.newast.2024.102296
Viktória Kecskeméthy , Amy Louca , Yamila Miguel
{"title":"Temporal variability in transmission spectra of H2-dominated exoplanets: The influence of thermal evolution and stellar irradiation on atmospheric composition","authors":"Viktória Kecskeméthy , Amy Louca , Yamila Miguel","doi":"10.1016/j.newast.2024.102296","DOIUrl":"10.1016/j.newast.2024.102296","url":null,"abstract":"<div><p>Planets and their host stars undergo evolutionary changes over time, resulting in variations in internal temperature and incoming radiation, which significantly impact the temperature structure and composition of their atmospheres. These evolving conditions give rise to distinctive features in planetary spectra that are observable only during specific stages of planetary evolution. We aim to understand how the composition of planets with H<sub>2</sub>-dominated atmospheres changes over longer timescales due to their thermal evolution. We also investigate time-dependent features in the transmission spectra. These features could provide insights in both the formation and evolution of these gaseous planets, as well as the timescales of these changes, enabling us to study the potential variability of exoplanets over time. We evolve a <span><math><mo>∼</mo></math></span>0.04 M<span><math><msub><mrow></mrow><mrow><mi>Jup</mi></mrow></msub></math></span> and <span><math><mo>∼</mo></math></span>0.45 M<span><math><msub><mrow></mrow><mrow><mi>Jup</mi></mrow></msub></math></span> planet around a 1.0 M<span><math><msub><mrow></mrow><mrow><mo>⊙</mo></mrow></msub></math></span> and 1.3 M<span><math><msub><mrow></mrow><mrow><mo>⊙</mo></mrow></msub></math></span> star respectively for 10<span><math><msup><mrow></mrow><mrow><mn>9</mn><mo>.</mo><mn>5</mn></mrow></msup></math></span> years. In both systems, the planets are considered at semi-major axes of 0.1 AU and 1.0 AU. The star-planet systems are evolved by making use of Modules for Experiments in Stellar Astrophysics (MESA). The temperature–pressure profiles are obtained at selected time-steps using an analytical approximation based on the internal and irradiation temperature of the planet at each time step. We then use VULCAN, a photochemical kinetics code, to see how the composition changes with time in the atmosphere due to the thermal evolution of the planets. By making use of the radiative transfer code petitRADTrans, we also simulate the evolution of the transmission spectra of the planets to find potential time-dependent spectral features. Our findings show a prominent change in the CO<span><math><msub><mrow></mrow><mrow><mn>2</mn></mrow></msub></math></span> feature at <span><math><mrow><mo>∼</mo><mn>4</mn><mo>.</mo><mn>3</mn><mi>μ</mi><mi>m</mi></mrow></math></span>. For the 0.45 M<span><math><msub><mrow></mrow><mrow><mi>Jup</mi></mrow></msub></math></span> case, this feature is visible in the pre-main-sequence phase of the host star, regardless of orbital distance from the host star. In the case of the <span><math><mo>∼</mo></math></span>0.04 M<span><math><msub><mrow></mrow><mrow><mi>Jup</mi></mrow></msub></math></span> planet, this CO<sub>2</sub> feature is visible until t <span><math><mo>≤</mo></math></span> 10<sup>6</sup> years, and then it reappears after t <span><math><mo>≥</mo></math></span> 10<sup>8</sup> years when the planet is 0.1 AU away the host star. The CH<sub>4</sub> features ","PeriodicalId":54727,"journal":{"name":"New Astronomy","volume":"113 ","pages":"Article 102296"},"PeriodicalIF":1.9,"publicationDate":"2024-08-21","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S1384107624001106/pdfft?md5=d658e35eb5e86085855c30c9d7f75b81&pid=1-s2.0-S1384107624001106-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142040012","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
Pulsation modes of three Delta Scuti stars using Kepler project data: KIC3429637, KIC10451090, KIC2987660 利用开普勒项目数据研究三颗德尔塔苏蒂星的脉动模式:KIC3429637、KIC10451090、KIC2987660
IF 1.9 4区 物理与天体物理
New Astronomy Pub Date : 2024-08-14 DOI: 10.1016/j.newast.2024.102294
Amin Shafaeiyeh Hiagh, Nematollah Riazi
{"title":"Pulsation modes of three Delta Scuti stars using Kepler project data: KIC3429637, KIC10451090, KIC2987660","authors":"Amin Shafaeiyeh Hiagh,&nbsp;Nematollah Riazi","doi":"10.1016/j.newast.2024.102294","DOIUrl":"10.1016/j.newast.2024.102294","url":null,"abstract":"<div><p>We have analyzed the light curves of three <span><math><mi>δ</mi></math></span> Scuti stars that were observed by the Kepler Space Telescope. Data collected by the Kepler space telescope, as well as analysis of the light curve of each star and the use of online databases, have been utilized to achieve the objectives of this project. Data has been collected through Kepler's main mission. We compare both data that we get from the Lightkurve package of Python and the KASOC online data centre to verify the data. We select the necessary data like flux, observation date, and the spectral type of the stars. By investigating various types of pulsating variable stars, three Delta Scuti stars have been selected due to their flux, pulsating type, etc. It is observed that most of these stars are pulsating in the p-modes. However, the selected stars pulsate in both p-modes and (possibly) g-modes. We select these stars, due to the lack of articles about them. Furthermore, some physical properties of these stars are deduced from their light curves. In summary, the results of this study indicate that the stars KIC3429637 and KIC10451090 are pulsating only in p-modes, while KIC2987660 is pulsating both in p-modes and g-modes.</p></div>","PeriodicalId":54727,"journal":{"name":"New Astronomy","volume":"113 ","pages":"Article 102294"},"PeriodicalIF":1.9,"publicationDate":"2024-08-14","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142075885","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
Combined light curve and radial velocity analysis of the neglected contact binary S Ant 被忽视的接触双星 S Ant 的综合光变曲线和径向速度分析
IF 1.9 4区 物理与天体物理
New Astronomy Pub Date : 2024-08-12 DOI: 10.1016/j.newast.2024.102291
Olivera Latković, Atila Čeki
{"title":"Combined light curve and radial velocity analysis of the neglected contact binary S Ant","authors":"Olivera Latković,&nbsp;Atila Čeki","doi":"10.1016/j.newast.2024.102291","DOIUrl":"10.1016/j.newast.2024.102291","url":null,"abstract":"<div><p>We present the first combined photometric and spectroscopic solution of the bright southern contact binary S Ant based on the <em>Transiting Exoplanet Survey Satellite</em> (TESS) light curve and the radial velocities from the David Dunlap Observatory survey. S Ant is a W UMa type binary in deep contact, with a mass ratio of 0.34 and a relatively massive and hot F-type primary. Beside the standard modeling of the phase-binned light curve, we also perform “seasonal modeling” where we treat each of the 83 orbital cycles present in the TESS data as a separate light curve. The resulting ensemble of solutions shows evidence of quasi-periodic migration of a long-lived, dark, polar spot. The migration is confirmed independently by eclipse time variations which display remarkably strong correlation with the spot location.</p></div>","PeriodicalId":54727,"journal":{"name":"New Astronomy","volume":"113 ","pages":"Article 102291"},"PeriodicalIF":1.9,"publicationDate":"2024-08-12","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141978307","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
The size and shape dependence of the SDSS galaxy bispectrum SDSS星系双谱的大小和形状依赖性
IF 1.9 4区 物理与天体物理
New Astronomy Pub Date : 2024-08-10 DOI: 10.1016/j.newast.2024.102292
Anindita Nandi , Sukhdeep Singh Gill , Debanjan Sarkar , Abinash Kumar Shaw , Biswajit Pandey , Somnath Bharadwaj
{"title":"The size and shape dependence of the SDSS galaxy bispectrum","authors":"Anindita Nandi ,&nbsp;Sukhdeep Singh Gill ,&nbsp;Debanjan Sarkar ,&nbsp;Abinash Kumar Shaw ,&nbsp;Biswajit Pandey ,&nbsp;Somnath Bharadwaj","doi":"10.1016/j.newast.2024.102292","DOIUrl":"10.1016/j.newast.2024.102292","url":null,"abstract":"&lt;div&gt;&lt;p&gt;We have measured the spherically averaged bispectrum of the SDSS main galaxy sample, considering a volume-limited &lt;span&gt;&lt;math&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mrow&gt;&lt;mo&gt;[&lt;/mo&gt;&lt;mn&gt;296&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;75&lt;/mn&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;mi&gt;Mpc&lt;/mi&gt;&lt;mo&gt;]&lt;/mo&gt;&lt;/mrow&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;3&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/math&gt;&lt;/span&gt; data cube with mean galaxy number density &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;63&lt;/mn&gt;&lt;mo&gt;×&lt;/mo&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mn&gt;10&lt;/mn&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;3&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;Mpc&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;3&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt; and median redshift &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;102&lt;/mn&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt;. Our analysis considers &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mo&gt;∼&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;37&lt;/mn&gt;&lt;mo&gt;×&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;8&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt; triangles, for which we have measured the binned bispectrum and analysed its dependence on the size and shape of the triangle. It spans wavenumbers &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;k&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;075&lt;/mn&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;434&lt;/mn&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;Mpc&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt; for equilateral triangles, and a smaller range of &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;k&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt; (the largest side) for triangles of other shapes. For all shapes, we find that the measured bispectrum is well modelled by a power law &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mi&gt;A&lt;/mi&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mrow&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;k&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;/&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;Mpc&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/mrow&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt;, where the best-fit values of &lt;span&gt;&lt;math&gt;&lt;mi&gt;A&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt; and &lt;span&gt;&lt;math&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt; vary with the shape. The parameter &lt;span&gt;&lt;math&gt;&lt;mi&gt;A&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt; is the minimum for equilateral triangles and increases as the shape is deformed to linear triangles where the two largest sides are nearly aligned, reaching its maximum value for &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mi&gt;μ&lt;/mi&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;95&lt;/mn&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;75&lt;/mn&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt;. The values of &lt;span&gt;&lt;math&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt; are all negative, &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt; is minimum &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mn&gt;3&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;12&lt;/mn&gt;&lt;mo&gt;±&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;35&lt;/mn&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt; for the shape bin &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mi&gt;μ&lt;/mi&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;65&lt;/mn&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;75&lt;/mn&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt;, and &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mn&gt;3&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;8&lt;/mn&gt;&lt;mo&gt;±&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;28&lt;/mn&gt;&lt;/mrow","PeriodicalId":54727,"journal":{"name":"New Astronomy","volume":"113 ","pages":"Article 102292"},"PeriodicalIF":1.9,"publicationDate":"2024-08-10","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142006419","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
Asteroseismology of evolved stars in six star clusters observed by Kepler/K2 开普勒/K2观测到的六个星团中的演化恒星的小行星动力学
IF 1.9 4区 物理与天体物理
New Astronomy Pub Date : 2024-07-27 DOI: 10.1016/j.newast.2024.102290
Yun-A Jo, Heon-Young Chang
{"title":"Asteroseismology of evolved stars in six star clusters observed by Kepler/K2","authors":"Yun-A Jo,&nbsp;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>&lt;</mo><msub><mrow><mi>ν</mi></mrow><mrow><mi>max</mi></mrow></msub><mo>&lt;</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}
引用次数: 0
Further lunar occultations results from the Trebur Observatory, 2021–24 2021-24 年特雷伯天文台的进一步月掩结果
IF 1.9 4区 物理与天体物理
New Astronomy Pub Date : 2024-07-27 DOI: 10.1016/j.newast.2024.102289
J.M. Ohlert , A. Richichi
{"title":"Further lunar occultations results from the Trebur Observatory, 2021–24","authors":"J.M. Ohlert ,&nbsp;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}
引用次数: 0
Wormholes in dwarf and spiral galactic halo regions 矮星系和螺旋星系晕区的虫洞
IF 1.9 4区 物理与天体物理
New Astronomy Pub Date : 2024-07-20 DOI: 10.1016/j.newast.2024.102288
Mehedi Kalam , Amir Ghari , Irina Radinschi , Hosein Haghi , Farook Rahaman , Tandrima Chowdhury
{"title":"Wormholes in dwarf and spiral galactic halo regions","authors":"Mehedi Kalam ,&nbsp;Amir Ghari ,&nbsp;Irina Radinschi ,&nbsp;Hosein Haghi ,&nbsp;Farook Rahaman ,&nbsp;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}
引用次数: 0
Definition of multispectral camera system parameters to model the asteroid 2001 SN263 确定多光谱摄像系统参数以模拟小行星 2001 Sn263
IF 1.9 4区 物理与天体物理
New Astronomy Pub Date : 2024-07-15 DOI: 10.1016/j.newast.2024.102287
Gabriela de Carvalho Assis Goulart , Thiago Statella , Rafael Sfair
{"title":"Definition of multispectral camera system parameters to model the asteroid 2001 SN263","authors":"Gabriela de Carvalho Assis Goulart ,&nbsp;Thiago Statella ,&nbsp;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}
引用次数: 0
Modeling compact stars with two fluids 用两种流体模拟紧凑恒星
IF 1.9 4区 物理与天体物理
New Astronomy Pub Date : 2024-07-11 DOI: 10.1016/j.newast.2024.102286
Pedro Mafa , Vishnu Kakkat , Amos Kubeka , Mantile Lekala
{"title":"Modeling compact stars with two fluids","authors":"Pedro Mafa ,&nbsp;Vishnu Kakkat ,&nbsp;Amos Kubeka ,&nbsp;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}
引用次数: 0
The role of radial viscosity force and anisotropic thermal conduction in hot accretion flow 热吸积流中径向粘滞力和各向异性热传导的作用
IF 1.9 4区 物理与天体物理
New Astronomy Pub Date : 2024-07-11 DOI: 10.1016/j.newast.2024.102276
Maryam Ghasemnezhad , Mohsen Khosravi
{"title":"The role of radial viscosity force and anisotropic thermal conduction in hot accretion flow","authors":"Maryam Ghasemnezhad ,&nbsp;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}
引用次数: 0
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