Pub Date : 2024-07-31DOI: 10.1007/s10511-024-09823-4
A. Alizadehsabegh, F. Lomoz, A. Poro, A. Narimani
Photometric data were used to perform the first light curve analysis of the V0610 Vir binary system. Observations and analysis were done in the form of the Binary Systems of South and North (BSN) Project. We extracted the minima from our observations and compiled the literature, which was few. Therefore, we performed computations using the reference ephemeris and presented a new ephemeris and O-C diagram with a linear fit. Light curve analysis was performed using the PHOEBE Python code and the Markov chain Monte Carlo (MCMC) approach. The assumption of a hot starspot was required due to the asymmetry in the light curve’s maxima. The analysis shows that V0610 Vir is a contact binary system with a fillout factor of 0.085, a mass ratio of 0.998, and an inclination of 70°.65. The absolute parameters of the system were estimated based on the Gaia DR3 parallax method. The results show that the system is a low-mass contact binary with a total mass lower than 0.8 M⨀. The location of the stars was shown in the M - L and M - R diagrams.
利用测光数据对 V0610 Vir 双星系统进行了首次光曲线分析。观测和分析是以南北双星系统(BSN)项目的形式进行的。我们从观测数据中提取了最小值,并对文献进行了汇编,但文献很少。因此,我们使用参考星历表进行了计算,并提出了新的星历表和线性拟合的 O-C 图。光曲线分析是使用 PHOEBE Python 代码和马尔可夫链蒙特卡罗(MCMC)方法进行的。由于光曲线的最大值不对称,需要假定存在热星斑。分析表明,V0610 Vir 是一个接触双星系统,填充因子为 0.085,质量比为 0.998,倾角为 70°.65。该系统的绝对参数是根据 Gaia DR3 视差法估算的。结果表明,该系统是一个低质量的接触双星,总质量低于 0.8 M⨀。恒星的位置显示在 M - L 和 M - R 图中。
{"title":"BSN: First Light Curve Study of the Low Mass Contact Binary V0610 Vir","authors":"A. Alizadehsabegh, F. Lomoz, A. Poro, A. Narimani","doi":"10.1007/s10511-024-09823-4","DOIUrl":"10.1007/s10511-024-09823-4","url":null,"abstract":"<p>Photometric data were used to perform the first light curve analysis of the V0610 Vir binary system. Observations and analysis were done in the form of the Binary Systems of South and North (BSN) Project. We extracted the minima from our observations and compiled the literature, which was few. Therefore, we performed computations using the reference ephemeris and presented a new ephemeris and O-C diagram with a linear fit. Light curve analysis was performed using the PHOEBE Python code and the Markov chain Monte Carlo (MCMC) approach. The assumption of a hot starspot was required due to the asymmetry in the light curve’s maxima. The analysis shows that V0610 Vir is a contact binary system with a fillout factor of 0.085, a mass ratio of 0.998, and an inclination of 70°.65. The absolute parameters of the system were estimated based on the Gaia DR3 parallax method. The results show that the system is a low-mass contact binary with a total mass lower than 0.8 M<sub>⨀</sub>. The location of the stars was shown in the M - L and M - R diagrams.</p>","PeriodicalId":479,"journal":{"name":"Astrophysics","volume":"67 2","pages":"128 - 139"},"PeriodicalIF":0.6,"publicationDate":"2024-07-31","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141869720","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 : 2024-05-17DOI: 10.1007/s10511-024-09818-1
Yu. A. Fursyak
Here, we performed a statistical analysis of the parameters describing the transverse component of the longitudinal magnetic field gradient (∇ ⊥B z ) in the active regions of the AR – the AR-averaged transverse component of the longitudinal magnetic field gradient <∇ ⊥B z >, the average transverse component of the longitudinal magnetic field gradient in the vicinity of a point with its maximum value <max∇ ⊥B z >, the maximum value of the transverse component of the longitudinal magnetic field gradient between pairs of spots in the AR max(∇ ⊥B z ) sp . For calculating the denoted parameters, magnetograms of the Bz -components of the magnetic field vector at the level of the Sun’s photosphere obtained by the Helioseismic and Magnetic Imager (HMI) on board the Solar Dynamics Observatory (SDO) are used. The statistical sample contains data on 75 ARs. The values of the analyzed parameters obtained over the time of monitoring are compared with the level of flare productivity of the AR (the flare index FI). It is shown that: 1. The (langle overline{{nabla }_{perp }{{varvec{B}}}_{z}}rangle ) -FI dependence (the overhead line denotes averaging over the time of monitoring the AR) is quadratic with a correlation coefficient k = 0.54 while the spread in values of the quantity (langle overline{{nabla }_{perp }{{varvec{B}}}_{z}}rangle ) is small (lying within a a range of 0.08-0.12 G km-1 for the overwhelming majority of the studied regions) and differs very little for regions with low and high flare productivity, which may be explained by the dependence of ∇ ⊥B z on the area of the AR. 2. The dependence (langle overline{{text{max}}{nabla }_{perp }{{varvec{B}}}_{z}}rangle ) -FI is quasilinear with a correlation coefficient k = 0.61. 3. The dependence (overline{{text{max}}{nabla }_{perp }{{varvec{B}}}_{z}}) -FI is linear with a correlation coefficient k = 0.63. 4. The threshold values of the analyzed parameters are found: for (langle overline{{nabla }_{perp }{{varvec{B}}}_{z}}rangle ) ≥ 0.078 G km-1, for (langle overline{{text{max}}{nabla }_{perp }{{varvec{B}}}_{z}}rangle ) ≥ 0.983 G km-1, and for the parameter max(∇ ⊥B z) sp ≥ 0.118G km-1. For lower values of the analyzed parameters, no x-ray flares were recorded in any of the ARs of the analyzed sample.
最大值点附近纵向磁场梯度的平均横向分量 <max∇⊥B z >,AR max(∇ ⊥B z ) sp 中点对点之间纵向磁场梯度横向分量的最大值。为了计算所标注的参数,使用了太阳动力学观测台(SDO)上的太阳地震和磁场成像仪(HMI)获得的太阳光层水平磁场矢量 B z 分量的磁图。统计样本包含 75 个 AR 的数据。将监测期间获得的分析参数值与 AR 的耀斑生产力水平(耀斑指数 FI)进行了比较。结果表明1.(langle overline{{nabla }_{perp }{{varvec{B}}}_{z}}rangle )-FI相关性(架空线表示在监测AR的时间内的平均值)是二次的,相关系数k = 0.54 而 (langle overline{{nabla }_{perp }{{varvec{B}}}_{z}}rangle )量值的差值很小(在 0.08-0.12 G km-1 的范围内),而且在耀斑生产率低和高的地区差别很小,这可以用 ∇ ⊥ B z 与 AR 面积的关系来解释。2.依赖关系((langle overline{{text{max}}{nabla }_{perp }{{varvec{B}}}_{z}}rangle )-FI 是准线性关系,相关系数 k = 0.61。3.依赖关系 (overline{{text{max}}{nabla }_{perp }{{{varvec{B}}}_{z}}) -FI 是线性的,相关系数 k = 0.63。4.找到了分析参数的临界值:对于 (angle overline{{nabla }_{perp }{{varvec{B}}}_{z}}rangle ) ≥ 0.078 G km-1, for (langle overline{{text{max}}{nabla }_{perp }{{{varvec{B}}}_{z}}rangle ) ≥ 0.983 G km-1, and for the parameter max(∇ ⊥ B z) sp ≥ 0.118G km-1.对于较低的分析参数值,分析样本中的任何一个AR都没有记录到X射线耀斑。
{"title":"Transverse Gradients of Longitudinal Magnetic Field in Active Regions with Different Levels of Flare Productivity. II. Statistical Analysis","authors":"Yu. A. Fursyak","doi":"10.1007/s10511-024-09818-1","DOIUrl":"10.1007/s10511-024-09818-1","url":null,"abstract":"<p>Here, we performed a statistical analysis of the parameters describing the transverse component of the longitudinal magnetic field gradient (∇ <sub>⊥</sub> <b><i>B </i></b><sub><i>z</i></sub> ) in the active regions of the AR – the AR-averaged transverse component of the longitudinal magnetic field gradient <∇ <sub>⊥</sub> <b><i>B z</i></b> >, the average transverse component of the longitudinal magnetic field gradient in the vicinity of a point with its maximum value <max∇ <sub>⊥</sub> <b><i>B z</i></b> >, the maximum value of the transverse component of the longitudinal magnetic field gradient between pairs of spots in the AR max(∇ <sub>⊥</sub> <b><i>B </i></b><sub><i>z</i></sub> ) <sub><i>sp</i></sub> . For calculating the denoted parameters, magnetograms of the <b><i>B</i></b> <sub>z</sub> -components of the magnetic field vector at the level of the Sun’s photosphere obtained by the Helioseismic and Magnetic Imager (HMI) on board the Solar Dynamics Observatory (SDO) are used. The statistical sample contains data on 75 ARs. The values of the analyzed parameters obtained over the time of monitoring are compared with the level of flare productivity of the AR (the flare index FI). It is shown that: 1. The <span>(langle overline{{nabla }_{perp }{{varvec{B}}}_{z}}rangle )</span> -FI dependence (the overhead line denotes averaging over the time of monitoring the AR) is quadratic with a correlation coefficient k = 0.54 while the spread in values of the quantity <span>(langle overline{{nabla }_{perp }{{varvec{B}}}_{z}}rangle )</span> is small (lying within a a range of 0.08-0.12 G km<sup>-1</sup> for the overwhelming majority of the studied regions) and differs very little for regions with low and high flare productivity, which may be explained by the dependence of ∇ <sub>⊥</sub> <b><i>B </i></b><sub><i>z</i></sub> on the area of the AR. 2. The dependence <span>(langle overline{{text{max}}{nabla }_{perp }{{varvec{B}}}_{z}}rangle )</span> -FI is quasilinear with a correlation coefficient k = 0.61. 3. The dependence <span>(overline{{text{max}}{nabla }_{perp }{{varvec{B}}}_{z}})</span> -FI is linear with a correlation coefficient k = 0.63. 4. The threshold values of the analyzed parameters are found: for <span>(langle overline{{nabla }_{perp }{{varvec{B}}}_{z}}rangle )</span> ≥ 0.078 G km<sup>-1</sup>, for <span>(langle overline{{text{max}}{nabla }_{perp }{{varvec{B}}}_{z}}rangle )</span> ≥ 0.983 G km<sup>-1</sup>, and for the parameter max(∇ <sub>⊥</sub> <b><i>B </i></b><sub><i>z</i></sub>) <sub><i>sp</i></sub> ≥ 0.118G km<sup>-1</sup>. For lower values of the analyzed parameters, no x-ray flares were recorded in any of the ARs of the analyzed sample.</p>","PeriodicalId":479,"journal":{"name":"Astrophysics","volume":"67 1","pages":"67 - 79"},"PeriodicalIF":0.6,"publicationDate":"2024-05-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140964523","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 : 2024-05-17DOI: 10.1007/s10511-024-09812-7
L. N. Kondratyeva, I. V. Reva, E. K. Denissyuk, S. A. Shomshekova, A. K. Aimanova
Photometric and spectral observations of 7 stars in the WC and WO sequences were made at the Fesenkov Astrophysical Institute in 2021-2022. These observations served as the basis of estimates of the brightness of the objects in BVRc filters and the absolute fluxes of radiation in the emission lines. Changes in the brightness of WR 121 over the limits of 0m.1-0m.15 were recorded. Changes in the fluxes of emission lines were detected in the spectra of several of the objects, WR 4, WR 5, WR 121, and WR 128.
{"title":"Photometric and Spectral Studies of a Group of Wolf-Rayet Galactic Stars. II. WC and WO Sequences","authors":"L. N. Kondratyeva, I. V. Reva, E. K. Denissyuk, S. A. Shomshekova, A. K. Aimanova","doi":"10.1007/s10511-024-09812-7","DOIUrl":"10.1007/s10511-024-09812-7","url":null,"abstract":"<p>Photometric and spectral observations of 7 stars in the WC and WO sequences were made at the Fesenkov Astrophysical Institute in 2021-2022. These observations served as the basis of estimates of the brightness of the objects in BVRc filters and the absolute fluxes of radiation in the emission lines. Changes in the brightness of WR 121 over the limits of 0<sup>m</sup>.1-0<sup>m</sup>.15 were recorded. Changes in the fluxes of emission lines were detected in the spectra of several of the objects, WR 4, WR 5, WR 121, and WR 128.</p>","PeriodicalId":479,"journal":{"name":"Astrophysics","volume":"67 1","pages":"9 - 23"},"PeriodicalIF":0.6,"publicationDate":"2024-05-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140964945","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 : 2024-05-17DOI: 10.1007/s10511-024-09814-5
Yu. V. Glagolevskij
Based on published data on the magnitudes of the magnetic field, models are constructed of several magnetic stars of different types of peculiarity and the parameters of the magnetic field are obtained. Among the hot objects, differences are also discovered in the physical conditions in the regions of the magnetic equators and in the region near the magnetic poles, which are not yet amenable to interpretation.
{"title":"Magnetic Field Structures of Chemically Peculiar Stars. II. HD98088, HD182180, HD221218, HD318107","authors":"Yu. V. Glagolevskij","doi":"10.1007/s10511-024-09814-5","DOIUrl":"10.1007/s10511-024-09814-5","url":null,"abstract":"<p>Based on published data on the magnitudes of the magnetic field, models are constructed of several magnetic stars of different types of peculiarity and the parameters of the magnetic field are obtained. Among the hot objects, differences are also discovered in the physical conditions in the regions of the magnetic equators and in the region near the magnetic poles, which are not yet amenable to interpretation.</p>","PeriodicalId":479,"journal":{"name":"Astrophysics","volume":"67 1","pages":"35 - 47"},"PeriodicalIF":0.6,"publicationDate":"2024-05-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141062255","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 : 2024-05-17DOI: 10.1007/s10511-024-09820-7
N. T. Karte, Kaplana Pawar, A. K. Dabre
The paper deals with the investigations of the behaviour and physical acceptability of the spatially homogeneous and isotropic FLRW space-time filled with pressureless matter and Rényi holographic dark energy under the Hubble's IR-cutoff in the framework of f (T, B) gravity. We have calculated some cosmological parameters to study the astrophysical consequences of the constructed model. We discussed their behaviour during the cosmic evolution, in particular, the statefinder and EoS parameters. It is found that the constructed Rényi holographic dark energy model travels from Phantom, ΛCDM, and lastly enters & remains in Quintessence dark energy era with the increase in redshift.
本文论述了在 f (T, B) 引力框架下,研究空间均匀和各向同性的 FLRW 时空的行为和物理可接受性,其中充满了无压物质和雷尼全息暗能量。我们计算了一些宇宙学参数,以研究构建模型的天体物理学后果。我们讨论了它们在宇宙演化过程中的表现,特别是状态探测器和 EoS 参数。研究发现,所构建的雷尼全息暗能量模型随着红移的增加,从幻影(Phantom)、ΛCDM,最后进入& 仍处于昆特塞斯(Quintessence)暗能量时代。
{"title":"Physical Acceptability of the Renyi Holographic Dark Energy Model Under the Hubble's Cutoff in f (T, B) Gravity","authors":"N. T. Karte, Kaplana Pawar, A. K. Dabre","doi":"10.1007/s10511-024-09820-7","DOIUrl":"10.1007/s10511-024-09820-7","url":null,"abstract":"<p>The paper deals with the investigations of the behaviour and physical acceptability of the spatially homogeneous and isotropic FLRW space-time filled with pressureless matter and Rényi holographic dark energy under the Hubble's IR-cutoff in the framework of f (T, B) gravity. We have calculated some cosmological parameters to study the astrophysical consequences of the constructed model. We discussed their behaviour during the cosmic evolution, in particular, the statefinder and EoS parameters. It is found that the constructed Rényi holographic dark energy model travels from Phantom, ΛCDM, and lastly enters & remains in Quintessence dark energy era with the increase in redshift.</p>","PeriodicalId":479,"journal":{"name":"Astrophysics","volume":"67 1","pages":"93 - 109"},"PeriodicalIF":0.6,"publicationDate":"2024-05-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141062302","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 : 2024-05-17DOI: 10.1007/s10511-024-09817-2
K. K. Gigoyan, K. S. Gigoyan, A. Sarkissian, M. Meftah, S. Bekki, E. Karapetyan, F. Rahmatullaeva, G. R. Kostandyan
Three new carbon C stars was confirmed among the sample of the Late-Type Stars candidates, selected on the Digitized First Byurakan Survey (DFBS) spectral plates. The DFBS is the digitized version of the First Byurakan Survey (FBS, or Markarian survey). The FBS was the first systematic survey of the extragalactic sky. This objective-prism survey was carried out in 1965-1980 by B.E.Markarian and his colleagues using the 1 m Schmidt telescope of the Byurakan Astrophysical Observatory and resulted in discovery of 1517 UV-excess (Markarian) galaxies. FBS spectral plates have been used long period to search and study faint LTS (C-type and M-type stars) at high Galactic latitudes. In this work we present Gaia DR3 photometric data, spectra, light curves, distances, high above/below Galactic plane, radial velocities (RV), and other important physical characteristics from the modern astronomical catalogues for three new confirmed DFBS C stars. The confirmation is based on Gaia DR3 BP/RP low-resolution spectral database. In our previous studies of the DFBS plates, these objects were presented as LTS candidates. One of the new confirmed objects is N-type C star, which is a Mira-type variable. Two remaining objects, are early CH-type giants at high Galactic latitudes. Most probably they present binary systems.
{"title":"The Digitized First Byurakan Survey Database Late-Type Stars Candidates. New Confirmations. II","authors":"K. K. Gigoyan, K. S. Gigoyan, A. Sarkissian, M. Meftah, S. Bekki, E. Karapetyan, F. Rahmatullaeva, G. R. Kostandyan","doi":"10.1007/s10511-024-09817-2","DOIUrl":"10.1007/s10511-024-09817-2","url":null,"abstract":"<p>Three new carbon C stars was confirmed among the sample of the Late-Type Stars candidates, selected on the Digitized First Byurakan Survey (DFBS) spectral plates. The DFBS is the digitized version of the First Byurakan Survey (FBS, or Markarian survey). The FBS was the first systematic survey of the extragalactic sky. This objective-prism survey was carried out in 1965-1980 by B.E.Markarian and his colleagues using the 1 m Schmidt telescope of the Byurakan Astrophysical Observatory and resulted in discovery of 1517 UV-excess (Markarian) galaxies. FBS spectral plates have been used long period to search and study faint LTS (C-type and M-type stars) at high Galactic latitudes. In this work we present Gaia DR3 photometric data, spectra, light curves, distances, high above/below Galactic plane, radial velocities (RV), and other important physical characteristics from the modern astronomical catalogues for three new confirmed DFBS C stars. The confirmation is based on Gaia DR3 BP/RP low-resolution spectral database. In our previous studies of the DFBS plates, these objects were presented as LTS candidates. One of the new confirmed objects is N-type C star, which is a Mira-type variable. Two remaining objects, are early CH-type giants at high Galactic latitudes. Most probably they present binary systems.</p>","PeriodicalId":479,"journal":{"name":"Astrophysics","volume":"67 1","pages":"60 - 66"},"PeriodicalIF":0.6,"publicationDate":"2024-05-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141064126","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 : 2024-05-17DOI: 10.1007/s10511-024-09811-8
A. M. Mickaelian, H. V. Abrahamyan, G. M. Paronyan, G. A. Mikayelyan, A. G. Sukiasyan, V. K. Mkrtchyan
We have carried out a spectral classification by the activity types for a subsample of blazars from the BZCAT v.5 Catalogue, namely the Flat Spectrum Radio Quasars (FSRQ) candidates, designated in the catalogue as BZQ subtype objects. The classification is based on the Sloan Digital Sky Survey (SDSS) homogeneous medium-resolution optical spectroscopy and along with the standard BPT-type diagnostic diagrams, we have applied our newly introduced fine classification scheme with subtypes of quasars and considering many more features. Out of 1909 BZQ objects, 618 having SDSS spectra were classified, resulting in 445 broad-line QSOs, 19 narrow-line QSOs, 138 broad-line Seyferts, 8 narrow-line Seyferts, and 2 Emission-line galaxies without a proper classification. We have calculated the absolute magnitudes and luminosities for all objects to distinguish QSOs from Seyferts, as defined by the Catalogue of QSOs and Active Galaxies, -22m.25 separation limit. This way 148 objects changed their BZCAT subtypes between BZQ to BZG, and also 6 BZQ objects to BZU.
{"title":"Classification of Flat Spectrum Radio Quasars by Optical Activity Types","authors":"A. M. Mickaelian, H. V. Abrahamyan, G. M. Paronyan, G. A. Mikayelyan, A. G. Sukiasyan, V. K. Mkrtchyan","doi":"10.1007/s10511-024-09811-8","DOIUrl":"10.1007/s10511-024-09811-8","url":null,"abstract":"<p>We have carried out a spectral classification by the activity types for a subsample of blazars from the BZCAT v.5 Catalogue, namely the Flat Spectrum Radio Quasars (FSRQ) candidates, designated in the catalogue as BZQ subtype objects. The classification is based on the Sloan Digital Sky Survey (SDSS) homogeneous medium-resolution optical spectroscopy and along with the standard BPT-type diagnostic diagrams, we have applied our newly introduced fine classification scheme with subtypes of quasars and considering many more features. Out of 1909 BZQ objects, 618 having SDSS spectra were classified, resulting in 445 broad-line QSOs, 19 narrow-line QSOs, 138 broad-line Seyferts, 8 narrow-line Seyferts, and 2 Emission-line galaxies without a proper classification. We have calculated the absolute magnitudes and luminosities for all objects to distinguish QSOs from Seyferts, as defined by the Catalogue of QSOs and Active Galaxies, -22<sup>m</sup>.25 separation limit. This way 148 objects changed their BZCAT subtypes between BZQ to BZG, and also 6 BZQ objects to BZU.</p>","PeriodicalId":479,"journal":{"name":"Astrophysics","volume":"67 1","pages":"1 - 8"},"PeriodicalIF":0.6,"publicationDate":"2024-05-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141062256","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 : 2024-05-17DOI: 10.1007/s10511-024-09819-0
B. C. Kalita, R. Kalita, S. Das
In this composition of plasma with negative dust charge, new classical distribution of nonthermal ions and Cairns distributed electrons, both supersonic and subsonic only rarefactive solitons are found to exist. It appears to conclude that the solitons cease to exist at the increase of c. The supersonic (M = 1.4) rarefactive solitons considerably and concavely increase from small amplitude with the increase of the ion to dust density ratio Q for various values of temperature α . The concave but increasing growth of amplitude of the rarefactive solitons for all M (>1) exhibits its distinct character. Smaller the Mach number (e.g., for M = 1.2), smaller is the amplitude of the solitons throughout the range of v0 (ion drift). The amplitudes of the rarefactive supersonic solitons are found to increase at the increase of the nonthermal parameter β for all r ( =ne0 /ni0 ). The dynamical scenario of this model indicates that the mass of the dusts should decrease in the plasma to generate higher amplitude solitons.
在这种带有负尘埃电荷、新经典分布的非热离子和凯恩斯分布电子的等离子体中,超音速和亚音速都只存在稀疏孤子。在不同温度值 α 下,超音速(M = 1.4)稀疏非活动孤子随着离子与尘埃密度比 Q 的增大而从小幅大幅凹增。在所有 M (>1) 条件下,稀有非活动孤子的振幅都呈凹形增长,但这种增长具有明显的特征。马赫数越小(如 M = 1.2),在整个 v0(离子漂移)范围内的孤子振幅就越小。在所有 r ( =ne0 /ni0 ) 条件下,稀疏超音速孤子的振幅随着非热参数 β 的增大而增大。该模型的动力学情景表明,等离子体中尘埃的质量应减少,以产生振幅更高的孤子。
{"title":"Dust Ion Acoustic Solitary Waves in Plasma with Cairns Distributed Electrons and New Classical Distribution of Ions","authors":"B. C. Kalita, R. Kalita, S. Das","doi":"10.1007/s10511-024-09819-0","DOIUrl":"10.1007/s10511-024-09819-0","url":null,"abstract":"<p>In this composition of plasma with negative dust charge, new classical distribution of nonthermal ions and Cairns distributed electrons, both supersonic and subsonic only rarefactive solitons are found to exist. It appears to conclude that the solitons cease to exist at the increase of <i>c</i>. The supersonic (<i>M</i> = 1.4) rarefactive solitons considerably and concavely increase from small amplitude with the increase of the ion to dust density ratio <i>Q</i> for various values of temperature α . The concave but increasing growth of amplitude of the rarefactive solitons for all <i>M</i> (>1) exhibits its distinct character. Smaller the Mach number (e.g., for <i>M</i> = 1.2), smaller is the amplitude of the solitons throughout the range of <i>v</i><sub>0</sub> (ion drift). The amplitudes of the rarefactive supersonic solitons are found to increase at the increase of the nonthermal parameter β for all <i>r</i> ( =<i>n</i><sub><i>e</i>0</sub> /<i>n</i><sub><i>i</i>0</sub> ). The dynamical scenario of this model indicates that the mass of the dusts should decrease in the plasma to generate higher amplitude solitons.</p>","PeriodicalId":479,"journal":{"name":"Astrophysics","volume":"67 1","pages":"80 - 92"},"PeriodicalIF":0.6,"publicationDate":"2024-05-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141064067","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 : 2024-05-17DOI: 10.1007/s10511-024-09816-3
E. S. Dmitrienko, I. S. Savanov
The properties of the planetary system TOI-1422, in which two planets of a neptune type orbit around a low-activity star of solar type with an age of about 5 billion years, are examined. We have previously analyzed activity of the star TOI-1422, found indications of the existence of possible activity cycles, and considered estimates of the orbital rotation period P of the star. The inner planet TOI-1422 b belongs to the hot-neptune types; it rotates with an orbit of period about 13 days and has an equilibrium temperature of Teq,b = 867 K. Calculations using a model of atmospheric loss with an energy limit for TOI-1422 b yielded 9.4·108 g/s of matter from the atmosphere. The outer planet of the system TOI-1422 c can also be regarded as a hot neptune; it has an orbital period of 29.3 days, its minimal mass, Mc sini, is 11.1M ⊕ , and the equilibrium temperature is Teq,c = 661 K. For estimating the radius of TOI-1422 c we have used an empirical M-R relation. It was found that the loss of matter from the atmosphere of the planet TOI-1422 c is 7.8·107 g/s and, given the error in the parameters, it may lie within a range from 6.1·107 g/s to 9.7·107 g/s.
在这个行星系统 TOI-1422 中,两颗海王星类型的行星围绕着一颗年龄约为 50 亿年的太阳型低活动恒星运行。我们之前分析了恒星 TOI-1422 的活动,发现了可能存在活动周期的迹象,并考虑了恒星轨道旋转周期 P 的估计值。内行星 TOI-1422 b 属于热海王星类型;它的公转轨道周期约为 13 天,平衡温度为 Teq,b = 867 K。该系统的外行星 TOI-1422 c 也可以被视为一颗热海王星;它的轨道周期为 29.3 天,最小质量 Mc sini 为 11.1M ⊕,平衡温度 Teq,c = 661 K。结果发现,TOI-1422 c行星大气中的物质损失为7.8-107克/秒,考虑到参数误差,可能在6.1-107克/秒到9.7-107克/秒之间。
{"title":"Mass Loss from the Atmosphere of the Planet TOI-1442 c","authors":"E. S. Dmitrienko, I. S. Savanov","doi":"10.1007/s10511-024-09816-3","DOIUrl":"10.1007/s10511-024-09816-3","url":null,"abstract":"<p>The properties of the planetary system TOI-1422, in which two planets of a neptune type orbit around a low-activity star of solar type with an age of about 5 billion years, are examined. We have previously analyzed activity of the star TOI-1422, found indications of the existence of possible activity cycles, and considered estimates of the orbital rotation period <i>P</i> of the star. The inner planet TOI-1422 b belongs to the hot-neptune types; it rotates with an orbit of period about 13 days and has an equilibrium temperature of <i>Teq,b</i> = 867 <i>K</i>. Calculations using a model of atmospheric loss with an energy limit for TOI-1422 b yielded 9.4·10<sup>8</sup> g/s of matter from the atmosphere. The outer planet of the system TOI-1422 c can also be regarded as a hot neptune; it has an orbital period of 29.3 days, its minimal mass, <i>Mc</i> sin<i>i</i>, is 11.1M <sub>⊕</sub> , and the equilibrium temperature is <i>Teq</i>,<i>c</i> = 661 <i>K</i>. For estimating the radius of TOI-1422 <i>c</i> we have used an empirical M-R relation. It was found that the loss of matter from the atmosphere of the planet TOI-1422 <i>c</i> is 7.8·10<sup>7</sup> g/s and, given the error in the parameters, it may lie within a range from 6.1·10<sup>7</sup> g/s to 9.7·10<sup>7</sup> g/s.</p>","PeriodicalId":479,"journal":{"name":"Astrophysics","volume":"67 1","pages":"54 - 59"},"PeriodicalIF":0.6,"publicationDate":"2024-05-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140963965","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 : 2024-05-17DOI: 10.1007/s10511-024-09815-4
I. S. Savanov
The properties of the planetary system TOI-784, in which an earth-like planet orbits a low-activity star of solar type, are examined. Archived V-band measurements of the brightness of TOI-784 in the ASAS 4 data base do not yield reliable indications about the variability of the brightness owing to rotation or about the cyclical long-term variability of this object. A possible estimate of the magnitude of the rotation period of the star is Prot/sini = 41.7 ± 11.4 days. The age of the system according to the empirical gyrochronological relations equals 7.8±3.4 billion years. The average value of the atmospheric activity parameter logR′HK = – 4.99 which corresponds to the level of low-activity stars with analogous (B-V) color index is found and is close to that of the sun. The radius of the planet TOI-784 b is equal to 1.93 R⊕, its mass is 9.67 M⊕, and its average density is 7.4 g/cm3 (the planet is rocky). An estimate of the loss of matter from the atmosphere of the planet TOI-784 b was obtained from an approximate formula corresponding to a model of loss by the atmosphere with a limit on energy. Calculations have shown that the rate of loss of matter by the atmosphere of the planet is 4.7 ⋅ 108 g/s. The relatively low rate of loss of matter by the planet’s atmosphere, despite a high effective temperature of the star’s atmosphere and the closeness of the planet to the star, is probably related to a low level of activity of the star.
{"title":"Activity of the Star TOI-784 and Loss of Atmospheric Mass by Its Planet","authors":"I. S. Savanov","doi":"10.1007/s10511-024-09815-4","DOIUrl":"10.1007/s10511-024-09815-4","url":null,"abstract":"<p>The properties of the planetary system TOI-784, in which an earth-like planet orbits a low-activity star of solar type, are examined. Archived V-band measurements of the brightness of TOI-784 in the ASAS 4 data base do not yield reliable indications about the variability of the brightness owing to rotation or about the cyclical long-term variability of this object. A possible estimate of the magnitude of the rotation period of the star is <i>Prot</i>/sini = 41.7 ± 11.4 days. The age of the system according to the empirical gyrochronological relations equals 7.8±3.4 billion years. The average value of the atmospheric activity parameter log<i>R</i>′<sub><i>HK</i></sub> = – 4.99 which corresponds to the level of low-activity stars with analogous (<i>B</i>-<i>V</i>) color index is found and is close to that of the sun. The radius of the planet TOI-784 b is equal to 1.93 <i>R</i><sub>⊕</sub>, its mass is 9.67 <i>M</i><sub>⊕</sub>, and its average density is 7.4 g/cm<sup>3</sup> (the planet is rocky). An estimate of the loss of matter from the atmosphere of the planet TOI-784 b was obtained from an approximate formula corresponding to a model of loss by the atmosphere with a limit on energy. Calculations have shown that the rate of loss of matter by the atmosphere of the planet is 4.7 ⋅ 10<sup>8</sup> g/s. The relatively low rate of loss of matter by the planet’s atmosphere, despite a high effective temperature of the star’s atmosphere and the closeness of the planet to the star, is probably related to a low level of activity of the star.</p>","PeriodicalId":479,"journal":{"name":"Astrophysics","volume":"67 1","pages":"48 - 53"},"PeriodicalIF":0.6,"publicationDate":"2024-05-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140964639","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}