Pub Date : 2025-08-21DOI: 10.1134/S1990341325600024
V. V. Bobylev, N. R. Ikhsanov, A. T. Bajkova
Four samples of open star clusters (OSCs) with average ages of 5.2, 18.6, 40, and 61 Myr have been analyzed. The selection of these OSCs was carried out from a narrow region inclined to the Galactic (Y) axis at an angle of (25^{circ}). Spectral analysis of the vertical positions and velocities of the selected clusters showed that the Radcliffe wave is associated with OSCs no older than 30 Myr. The following estimates of the Radcliffe wave characteristics were obtained for the OSCs with an average age of 5.2 Myr: (z_{textrm{max}}=117pm 12) pc with the wavelength (lambda=4.55pm 0.14) kpc, and the vertical velocity disturbance amplitude (W_{textrm{max}}=4.86pm 0.19) km s({}^{-1}) with the wavelength (lambda=1.74pm 0.08) kpc. For the OSCs with an average age of 18.6 Myr, the estimates are as follows: (z_{textrm{max}}=54pm 5) pc and (lambda=6.30pm 0.12) kpc, and the vertical velocity disturbance amplitude (W_{textrm{max}}=7.90pm 0.16) km s({}^{-1}) and (lambda=0.83pm 0.11) kpc. The radial motion of the Radcliffe wave away from the Galactic center has been confirmed. The velocity of such movement is 10 pc Myr({}^{-1}). In our opinion, the spatial distribution of OSCs younger than 30 Myr does not contradict the hypothesis of the association of the Radcliffe wave with the impact of shock waves from supernova explosions that arose on an extended front comparable in scale to the entire wave, that is, about 2 kpc in size.
{"title":"Age Estimation of the Radcliffe Wave from Open Star Clusters","authors":"V. V. Bobylev, N. R. Ikhsanov, A. T. Bajkova","doi":"10.1134/S1990341325600024","DOIUrl":"10.1134/S1990341325600024","url":null,"abstract":"<p>Four samples of open star clusters (OSCs) with average ages of 5.2, 18.6, 40, and 61 Myr have been analyzed. The selection of these OSCs was carried out from a narrow region inclined to the Galactic <span>(Y)</span> axis at an angle of <span>(25^{circ})</span>. Spectral analysis of the vertical positions and velocities of the selected clusters showed that the Radcliffe wave is associated with OSCs no older than 30 Myr. The following estimates of the Radcliffe wave characteristics were obtained for the OSCs with an average age of 5.2 Myr: <span>(z_{textrm{max}}=117pm 12)</span> pc with the wavelength <span>(lambda=4.55pm 0.14)</span> kpc, and the vertical velocity disturbance amplitude <span>(W_{textrm{max}}=4.86pm 0.19)</span> km s<span>({}^{-1})</span> with the wavelength <span>(lambda=1.74pm 0.08)</span> kpc. For the OSCs with an average age of 18.6 Myr, the estimates are as follows: <span>(z_{textrm{max}}=54pm 5)</span> pc and <span>(lambda=6.30pm 0.12)</span> kpc, and the vertical velocity disturbance amplitude <span>(W_{textrm{max}}=7.90pm 0.16)</span> km s<span>({}^{-1})</span> and <span>(lambda=0.83pm 0.11)</span> kpc. The radial motion of the Radcliffe wave away from the Galactic center has been confirmed. The velocity of such movement is 10 pc Myr<span>({}^{-1})</span>. In our opinion, the spatial distribution of OSCs younger than 30 Myr does not contradict the hypothesis of the association of the Radcliffe wave with the impact of shock waves from supernova explosions that arose on an extended front comparable in scale to the entire wave, that is, about 2 kpc in size.</p>","PeriodicalId":478,"journal":{"name":"Astrophysical Bulletin","volume":"80 2","pages":"181 - 189"},"PeriodicalIF":1.4,"publicationDate":"2025-08-21","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"144888023","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 : 2025-08-21DOI: 10.1134/S1990341325600255
M. A. Burlak, K. N. Grankin, A. V. Dodin, A. V. Zharova, N. P. Ikonnikova, V. A. Kiryukhina, S. A. Lamzin, B. S. Safonov, I. A. Strakhov
We have constructed and analyzed the secular light curve of BP Tau, a classical T Tau star. Wave-like variations in the average brightness level of the star with an amplitude of (Delta Bapprox 0overset{textrm{m}}{.}2) and a characteristic time of several decades were found. We present arguments in favor of the concept that three deep ((Delta Bsim 1overset{textrm{m}}{.}5)) dimming episodes lasting from one hour to several days are associated with the eclipse of a hot (accretion) spot by the dust infalling on the star along with gas. It is possible that such eclipses, albeit with a smaller amplitude, are the reason for the lack in BP Tau of a strictly expressed brightness variation periodicity related to axial rotation. We found that in the distance range of 0.1 to 200 AU, BP Tau has no companions with masses greater than (0.2;M_{odot}). Possible reasons of brightness and color index variability of the star on different time scales are discussed.
{"title":"On the Causes of Brightness Variability of a Young Star BP Tau","authors":"M. A. Burlak, K. N. Grankin, A. V. Dodin, A. V. Zharova, N. P. Ikonnikova, V. A. Kiryukhina, S. A. Lamzin, B. S. Safonov, I. A. Strakhov","doi":"10.1134/S1990341325600255","DOIUrl":"10.1134/S1990341325600255","url":null,"abstract":"<p>We have constructed and analyzed the secular light curve of BP Tau, a classical T Tau star. Wave-like variations in the average brightness level of the star with an amplitude of <span>(Delta Bapprox 0overset{textrm{m}}{.}2)</span> and a characteristic time of several decades were found. We present arguments in favor of the concept that three deep <span>((Delta Bsim 1overset{textrm{m}}{.}5))</span> dimming episodes lasting from one hour to several days are associated with the eclipse of a hot (accretion) spot by the dust infalling on the star along with gas. It is possible that such eclipses, albeit with a smaller amplitude, are the reason for the lack in BP Tau of a strictly expressed brightness variation periodicity related to axial rotation. We found that in the distance range of 0.1 to 200 AU, BP Tau has no companions with masses greater than <span>(0.2;M_{odot})</span>. Possible reasons of brightness and color index variability of the star on different time scales are discussed.</p>","PeriodicalId":478,"journal":{"name":"Astrophysical Bulletin","volume":"80 2","pages":"279 - 293"},"PeriodicalIF":1.4,"publicationDate":"2025-08-21","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"144888030","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 : 2025-08-21DOI: 10.1134/S1990341325600103
A. S. Rastorguev, M. V. Zabolotskikh, N. N. Samus, N. A. Gorynya
A revision of the orbital parameters of the spectroscopic binary Cepheid TX Del, often classified as a BL Her subtype of T2 variables, has been carried out. The pulsation radius is determined from two series of photometric observations, including Gaia DR3: (langle Rrangleapprox 22.4pm 0.8,R_{odot}) for the ((B,V)) bands and (langle Rrangleapprox 20.6pm 0.6,R_{odot}) for the ((BP,RP)) bands, respectively. The amplitude of the radius variations is about (2,R_{odot}). The new radius estimates are significantly smaller than the previous estimates, which were in the range of 37 to 60 (R_{odot}). Using the Bayesian distance, (langle Drangleapprox 1064pm 25) pc, the absolute values of TX Del are estimated to be (langle M_{V}rangle_{I}approx{-}1.31pm 0.04) mag and (langle M_{G}rangle_{I}approx{-}1.40pm 0.03) mag, respectively. The absolute magnitude and mean radius of TX Del are in excellent agreement with the predictions of the ‘‘period–luminosity’’ and ‘‘period–radius’’ relations for T2 Cepheids with a period of (P_{textrm{pls}}approx 6.1662) days; TX Del is approximately (2overset{textrm{m}}{.}2) fainter than classical Cepheids with the same period. It is shown that for orbital plane inclination angles (20^{circ}<i<(30{-}35)^{circ}) the satellite can be more massive than the main component, which leads to an evolutionary scenario with mass exchange. The current Roche sphere filling degree is (37{-}55%). The orbit of the binary system TX Del calculated based on astrometric data from Gaia DR3 and radial velocity is limited by a (|z|<0.42) kpc torus with the inner and outer radii equal to 7.2 and 8.3 kpc, respectively, while the vertical velocity is (|V_{z}|leq 38) km s({}^{-1}); the period of galactovertical oscillations is about 77 Myrs. The tangential velocity is 220–255 km s({}^{-1}). The high metallicity and kinematic characteristics allow us to refer TX Del to the population of the old disk of the Milky Way with a vertical scale (H_{z}approx 0.3) kpc (or to a thick disk with (H_{z}approx 0.85) kpc). At the same time, in terms of pulsation characteristics (period, luminosity, and position in the instability strip), TX Del is close to Population II Cepheids with (textrm{[Fe/H]}<{-}1) (including globular cluster Cepheids) that are at the evolutionary stage after the horizontal branch. To finally clarify the evolutionary status of such variables, additional evolutionary and pulsation calculations are required over a wider range of periods and luminosities.
{"title":"Orbital Parameters, Radius and Classification of the Spectroscopic Binary Cepheid TX Del Based on Gaia DR3 Data","authors":"A. S. Rastorguev, M. V. Zabolotskikh, N. N. Samus, N. A. Gorynya","doi":"10.1134/S1990341325600103","DOIUrl":"10.1134/S1990341325600103","url":null,"abstract":"<p>A revision of the orbital parameters of the spectroscopic binary Cepheid TX Del, often classified as a BL Her subtype of T2 variables, has been carried out. The pulsation radius is determined from two series of photometric observations, including Gaia DR3: <span>(langle Rrangleapprox 22.4pm 0.8,R_{odot})</span> for the (<span>(B,V)</span>) bands and <span>(langle Rrangleapprox 20.6pm 0.6,R_{odot})</span> for the (<span>(BP,RP)</span>) bands, respectively. The amplitude of the radius variations is about <span>(2,R_{odot})</span>. The new radius estimates are significantly smaller than the previous estimates, which were in the range of 37 to 60 <span>(R_{odot})</span>. Using the Bayesian distance, <span>(langle Drangleapprox 1064pm 25)</span> pc, the absolute values of TX Del are estimated to be <span>(langle M_{V}rangle_{I}approx{-}1.31pm 0.04)</span> mag and <span>(langle M_{G}rangle_{I}approx{-}1.40pm 0.03)</span> mag, respectively. The absolute magnitude and mean radius of TX Del are in excellent agreement with the predictions of the ‘‘period–luminosity’’ and ‘‘period–radius’’ relations for T2 Cepheids with a period of <span>(P_{textrm{pls}}approx 6.1662)</span> days; TX Del is approximately <span>(2overset{textrm{m}}{.}2)</span> fainter than classical Cepheids with the same period. It is shown that for orbital plane inclination angles <span>(20^{circ}<i<(30{-}35)^{circ})</span> the satellite can be more massive than the main component, which leads to an evolutionary scenario with mass exchange. The current Roche sphere filling degree is <span>(37{-}55%)</span>. The orbit of the binary system TX Del calculated based on astrometric data from Gaia DR3 and radial velocity is limited by a <span>(|z|<0.42)</span> kpc torus with the inner and outer radii equal to 7.2 and 8.3 kpc, respectively, while the vertical velocity is <span>(|V_{z}|leq 38)</span> km s<span>({}^{-1})</span>; the period of galactovertical oscillations is about 77 Myrs. The tangential velocity is 220–255 km s<span>({}^{-1})</span>. The high metallicity and kinematic characteristics allow us to refer TX Del to the population of the old disk of the Milky Way with a vertical scale <span>(H_{z}approx 0.3)</span> kpc (or to a thick disk with <span>(H_{z}approx 0.85)</span> kpc). At the same time, in terms of pulsation characteristics (period, luminosity, and position in the instability strip), TX Del is close to Population II Cepheids with <span>(textrm{[Fe/H]}<{-}1)</span> (including globular cluster Cepheids) that are at the evolutionary stage after the horizontal branch. To finally clarify the evolutionary status of such variables, additional evolutionary and pulsation calculations are required over a wider range of periods and luminosities.</p>","PeriodicalId":478,"journal":{"name":"Astrophysical Bulletin","volume":"80 2","pages":"242 - 253"},"PeriodicalIF":1.4,"publicationDate":"2025-08-21","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"144887998","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 : 2025-08-21DOI: 10.1134/S1990341325600140
A. M. Melnik, E. N. Podzolkova
We study the formation of the Hercules stream in the model Galactic disk which includes the outer resonance ring (R_{1}R_{2}) located near the Outer Lindblad Resonance (OLR) of the bar. The Hercules region and the anti-Hercules region, introduced for calibration, were restricted in space by the solar neighbourhood (r<0.5) kpc, and on the ((V_{R}), (V_{T})) plane by ellipses centered at (V_{R}=25) km s({}^{-1}) and (V_{T}=200) km s({}^{-1}) (Hercules), and at (V_{R}=-25) km s({}^{-1}) and (V_{T}=200) km s({}^{-1}) (anti-Hercules). The number of stars in the Hercules region reaches a maximum in the time period of (2-3) Gyr from the start of simulation and the number of stars in the anti-Hercules region oscillates with a period of (1.8pm 0.1) Gyr. The majority of stars in the model disk located in the Hercules and anti-Hercules regions have orbits elongated perpendicular and parallel to the bar, respectively. The median value of the initial distances of stars in the Hercules (anti-Hercules) region is slightly smaller (larger) than the OLR radius, respectively. There are two types of orbits in the Hercules region. Orbits of the first type always lie inside a figure bounded by two ellipses elongated perpendicular to the bar. Orbits of the second type are elongated at the angles of (-60^{circ}) or (60^{circ}) to the major axis of the bar most of the time. The distribution of stars in the Hercules region along the period of slow oscillations in the angular momentum has two maxima: (P=0.7) and 2.6 Gyr corresponding to orbits of the first and second type. In the anti-Hercules region, most orbits are captured by libration relative to the major axis of the bar with a period of 1.9 Gyr. In general, orbits in the Hercules and anti-Hercules regions support the outer rings (R_{1}) and (R_{2}) elongated perpendicular and parallel to the bar, respectively. Stars from the Gaia DR3 catalog located in the Hercules region appear to be, on average, brighter, bluer, and more luminous than stars in the anti-Hercules region which is probably caused by selection effects due to different distributions of these stellar samples over the Galactic latitude (b).
我们研究了包含外共振环的模型银盘中大力神流的形成 (R_{1}R_{2}) 位于酒吧的外林德布莱德共振(OLR)附近。为了校准而引入的大力神区域和反大力神区域在空间上受到太阳邻域的限制 (r<0.5) ,并在((V_{R}), (V_{T})的椭圆平面 (V_{R}=25) Km s({}^{-1}) 和 (V_{T}=200) Km s({}^{-1}) (赫拉克勒斯)和at (V_{R}=-25) Km s({}^{-1}) 和 (V_{T}=200) Km s({}^{-1}) (反赫拉克勒斯)。大力神区域的恒星数量在大约的时间内达到最大值 (2-3) Gyr从模拟开始,反大力神区域的恒星数量以周期振荡 (1.8pm 0.1) Gyr。位于大力神星和反大力神星区域的模型盘中的大多数恒星的轨道分别垂直于和平行于条形结构。大力神星(反大力神星)区域内恒星的初始距离中值分别略小于(大于)OLR半径。大力神星区域有两种类型的轨道。第一种类型的轨道总是位于一个图形内,这个图形由两个垂直于条的椭圆所包围。第二类的轨道以的角度被拉长 (-60^{circ}) 或 (60^{circ}) 大部分时间都在杆的长轴上。大力神星区恒星沿角动量慢振荡周期的分布有两个极大值: (P=0.7) 和2.6 Gyr分别对应第一类和第二类轨道。在反大力神星区域,大多数轨道是通过相对于长轴的振动捕获的,周期为1.9 Gyr。一般来说,大力神星和反大力神星区域的轨道支持外环 (R_{1}) 和 (R_{2}) 细长的,垂直的,平行于杆的。位于大力神区域的盖亚DR3星表中的恒星平均而言似乎比位于反大力神区域的恒星更亮、更蓝、更亮,这可能是由于这些恒星样本在银河系纬度上的不同分布所造成的选择效应 (b).
{"title":"Hercules Stream and the Outer Elliptical Ring (boldsymbol{R_{1}R_{2}})","authors":"A. M. Melnik, E. N. Podzolkova","doi":"10.1134/S1990341325600140","DOIUrl":"10.1134/S1990341325600140","url":null,"abstract":"<p>We study the formation of the Hercules stream in the model Galactic disk which includes the outer resonance ring <span>(R_{1}R_{2})</span> located near the Outer Lindblad Resonance (OLR) of the bar. The Hercules region and the anti-Hercules region, introduced for calibration, were restricted in space by the solar neighbourhood <span>(r<0.5)</span> kpc, and on the (<span>(V_{R})</span>, <span>(V_{T})</span>) plane by ellipses centered at <span>(V_{R}=25)</span> km s<span>({}^{-1})</span> and <span>(V_{T}=200)</span> km s<span>({}^{-1})</span> (Hercules), and at <span>(V_{R}=-25)</span> km s<span>({}^{-1})</span> and <span>(V_{T}=200)</span> km s<span>({}^{-1})</span> (anti-Hercules). The number of stars in the Hercules region reaches a maximum in the time period of <span>(2-3)</span> Gyr from the start of simulation and the number of stars in the anti-Hercules region oscillates with a period of <span>(1.8pm 0.1)</span> Gyr. The majority of stars in the model disk located in the Hercules and anti-Hercules regions have orbits elongated perpendicular and parallel to the bar, respectively. The median value of the initial distances of stars in the Hercules (anti-Hercules) region is slightly smaller (larger) than the OLR radius, respectively. There are two types of orbits in the Hercules region. Orbits of the first type always lie inside a figure bounded by two ellipses elongated perpendicular to the bar. Orbits of the second type are elongated at the angles of <span>(-60^{circ})</span> or <span>(60^{circ})</span> to the major axis of the bar most of the time. The distribution of stars in the Hercules region along the period of slow oscillations in the angular momentum has two maxima: <span>(P=0.7)</span> and 2.6 Gyr corresponding to orbits of the first and second type. In the anti-Hercules region, most orbits are captured by libration relative to the major axis of the bar with a period of 1.9 Gyr. In general, orbits in the Hercules and anti-Hercules regions support the outer rings <span>(R_{1})</span> and <span>(R_{2})</span> elongated perpendicular and parallel to the bar, respectively. Stars from the Gaia DR3 catalog located in the Hercules region appear to be, on average, brighter, bluer, and more luminous than stars in the anti-Hercules region which is probably caused by selection effects due to different distributions of these stellar samples over the Galactic latitude <span>(b)</span>.</p>","PeriodicalId":478,"journal":{"name":"Astrophysical Bulletin","volume":"80 2","pages":"254 - 273"},"PeriodicalIF":1.4,"publicationDate":"2025-08-21","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"144888028","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 : 2025-08-21DOI: 10.1134/S1990341323600448
I. U. Tadjibaev, S. N. Nuritdinov, A. U. Omonov
In this paper we discuss the problems of classification of globular cluster systems (GCS), in particular, the problem of the auxiliary parameter. The simplest methods of their classification are proposed. The possibilities of classification by the degree of concentration of GCS to the center of the galaxy and the use of the velocity anisotropy parameter are studied. Empirical relationships between the initial value of the virial parameter and the physical characteristics of GCSs are found. It is shown that GCSs can be classified using the initial value of the virial parameter.
{"title":"On the Problems of Classification of Globular Cluster Systems","authors":"I. U. Tadjibaev, S. N. Nuritdinov, A. U. Omonov","doi":"10.1134/S1990341323600448","DOIUrl":"10.1134/S1990341323600448","url":null,"abstract":"<p>In this paper we discuss the problems of classification of globular cluster systems (GCS), in particular, the problem of the auxiliary parameter. The simplest methods of their classification are proposed. The possibilities of classification by the degree of concentration of GCS to the center of the galaxy and the use of the velocity anisotropy parameter are studied. Empirical relationships between the initial value of the virial parameter and the physical characteristics of GCSs are found. It is shown that GCSs can be classified using the initial value of the virial parameter.</p>","PeriodicalId":478,"journal":{"name":"Astrophysical Bulletin","volume":"80 2","pages":"202 - 208"},"PeriodicalIF":1.4,"publicationDate":"2025-08-21","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"144888025","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 : 2025-08-21DOI: 10.1134/S1990341325600152
M. L. Ostashova, A. S. Rastorguev
In this paper, we study the distribution law of the random force modulus in the nearest neighbor approximation (generalized Holtsmark distribution) and the asymptotic behavior of the Holtsmark distribution for large random forces for a fractal stellar medium in the solar neighborhood. The role of collisional processes and random forces in the dynamics of stellar systems is considered. This study is based on the investigation of the spatial distribution of 200 000 stars of all spectral classes at distances from 1 to 100 pc from the Sun according to Gaia DR2 data, the results of which indicate the presence of fractal structures in the solar neighborhood with a fractal dimension of (Dsimeq 2.41). The asymptotic distribution of random force derived for a fractal stellar medium demonstrates the important role of strong fields, with the magnitude of the random force decreasing somewhat more slowly compared to its distribution for a homogeneous medium.
{"title":"Fractal Distribution of Stars in the Solar Neighborhood and Random Forces","authors":"M. L. Ostashova, A. S. Rastorguev","doi":"10.1134/S1990341325600152","DOIUrl":"10.1134/S1990341325600152","url":null,"abstract":"<p>In this paper, we study the distribution law of the random force modulus in the nearest neighbor approximation (generalized Holtsmark distribution) and the asymptotic behavior of the Holtsmark distribution for large random forces for a fractal stellar medium in the solar neighborhood. The role of collisional processes and random forces in the dynamics of stellar systems is considered. This study is based on the investigation of the spatial distribution of 200 000 stars of all spectral classes at distances from 1 to 100 pc from the Sun according to Gaia DR2 data, the results of which indicate the presence of fractal structures in the solar neighborhood with a fractal dimension of <span>(Dsimeq 2.41)</span>. The asymptotic distribution of random force derived for a fractal stellar medium demonstrates the important role of strong fields, with the magnitude of the random force decreasing somewhat more slowly compared to its distribution for a homogeneous medium.</p>","PeriodicalId":478,"journal":{"name":"Astrophysical Bulletin","volume":"80 2","pages":"274 - 278"},"PeriodicalIF":1.4,"publicationDate":"2025-08-21","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"144888029","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 : 2025-08-21DOI: 10.1134/S1990341325600231
Yu. Yu. Glagolevskij, A. F. Nazarenko
The structure of the magnetic field of HD 37479 corresponds to the structure of a dipole displaced along the axis by a significant value (Delta a=0.2R_{*}) and across the axis by the value (Delta a=0.05R_{*}). As a result, the magnetic field is distributed extremely unevenly over the stellar surface. The maximum values of the average surface magnetic field are equal to (B_{s}=+2591) and (-7486) G. It is in these areas that the maximum wind occurs, and also in approximately these same areas the maximum helium abundance is observed. A cloud of rarefied gas extends along the magnetic equator, in which H(alpha) emission lines are formed.
HD 37479的磁场结构与偶极子的结构相对应,偶极子沿轴方向偏移了一个显著值(Delta a=0.2R_{*}),沿轴方向偏移了一个显著值(Delta a=0.05R_{*})。因此,磁场在恒星表面的分布极不均匀。平均表面磁场的最大值等于(B_{s}=+2591)和(-7486) G.正是在这些区域出现了最大的风,并且在大约相同的区域也观察到最大的氦丰度。稀薄的气体云沿着磁赤道延伸,在磁赤道形成了H (alpha)发射线。
{"title":"Special Features of the Magnetic Field Structure of the He-r Star HD 37479 (boldsymbol{sigma})Ori E","authors":"Yu. Yu. Glagolevskij, A. F. Nazarenko","doi":"10.1134/S1990341325600231","DOIUrl":"10.1134/S1990341325600231","url":null,"abstract":"<p>The structure of the magnetic field of HD 37479 corresponds to the structure of a dipole displaced along the axis by a significant value <span>(Delta a=0.2R_{*})</span> and across the axis by the value <span>(Delta a=0.05R_{*})</span>. As a result, the magnetic field is distributed extremely unevenly over the stellar surface. The maximum values of the average surface magnetic field are equal to <span>(B_{s}=+2591)</span> and <span>(-7486)</span> G. It is in these areas that the maximum wind occurs, and also in approximately these same areas the maximum helium abundance is observed. A cloud of rarefied gas extends along the magnetic equator, in which H<span>(alpha)</span> emission lines are formed.</p>","PeriodicalId":478,"journal":{"name":"Astrophysical Bulletin","volume":"80 2","pages":"190 - 201"},"PeriodicalIF":1.4,"publicationDate":"2025-08-21","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"144888024","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 : 2025-08-21DOI: 10.1134/S1990341324600704
A. M. H. Ahmed, A. R. Youssef, M. S. El-Nawawy, W. H. Elsanhoury
The study presents both photometric and kinematic Gaia DR3 analyses of the nonrelaxed open cluster Stock 3, which is found to be located at a distance of (2.95pm 0.70) kpc and to have an age of (16pm 4) Myr. We analyze the data to infer the cluster membership and thus determine the total mass, initial mass function, and the dynamical and kinematical status.
{"title":"Deep Photometric and Astrometric Investigation of the Non-relaxed Star Cluster Stock 3 Using Gaia DR3","authors":"A. M. H. Ahmed, A. R. Youssef, M. S. El-Nawawy, W. H. Elsanhoury","doi":"10.1134/S1990341324600704","DOIUrl":"10.1134/S1990341324600704","url":null,"abstract":"<p>The study presents both photometric and kinematic Gaia DR3 analyses of the nonrelaxed open cluster Stock 3, which is found to be located at a distance of <span>(2.95pm 0.70)</span> kpc and to have an age of <span>(16pm 4)</span> Myr. We analyze the data to infer the cluster membership and thus determine the total mass, initial mass function, and the dynamical and kinematical status.</p>","PeriodicalId":478,"journal":{"name":"Astrophysical Bulletin","volume":"80 2","pages":"209 - 222"},"PeriodicalIF":1.4,"publicationDate":"2025-08-21","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"144888026","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 : 2025-08-21DOI: 10.1134/S1990341325600176
A. V. Larichev, E. A. Kopylov, A. S. Goncharov, L. A. Bolbasova, V. P. Lukin, N. G. Iroshnikov, M. E. Sachkov
In this paper, we describe the design and technical features of the Rayleigh laser guide star (LGS) system as a reference source of the adaptive optics system (AOS) intended for use at the Zeiss-2000 telescope of the Terskol Peak Astronomical Observatory (coordinates (43overset{circ}{.}27631) N, (42overset{circ}{.}49939) E) located at an altitude of 3150 m above sea level. Experimental testing of the Rayleigh LGS system at the Zeiss-2000 telescope was carried out. The presented numerical estimates of the correlation radius (r_{0}) show that in the future, the use of an AOS with a Rayleigh LGS at this telescope will improve the quality of the formed image by an order of magnitude.
本文介绍了位于海拔3150 m的Terskol峰天文台(坐标(43overset{circ}{.}27631) N, (42overset{circ}{.}49939) E)蔡司-2000望远镜自适应光学系统(AOS)的参考光源瑞利激光导星(LGS)系统的设计和技术特点。在蔡司-2000望远镜上对瑞利LGS系统进行了实验测试。给出的相关半径(r_{0})的数值估计表明,在未来,在该望远镜上使用AOS和瑞利LGS将使形成的图像质量提高一个数量级。
{"title":"Parameters of Formation of Rayleigh Laser Guide Star System of Adaptive Optics for Zeiss-2000 Telescope of Terskol Peak Observatory","authors":"A. V. Larichev, E. A. Kopylov, A. S. Goncharov, L. A. Bolbasova, V. P. Lukin, N. G. Iroshnikov, M. E. Sachkov","doi":"10.1134/S1990341325600176","DOIUrl":"10.1134/S1990341325600176","url":null,"abstract":"<p>In this paper, we describe the design and technical features of the Rayleigh laser guide star (LGS) system as a reference source of the adaptive optics system (AOS) intended for use at the Zeiss-2000 telescope of the Terskol Peak Astronomical Observatory (coordinates <span>(43overset{circ}{.}27631)</span> N, <span>(42overset{circ}{.}49939)</span> E) located at an altitude of 3150 m above sea level. Experimental testing of the Rayleigh LGS system at the Zeiss-2000 telescope was carried out. The presented numerical estimates of the correlation radius <span>(r_{0})</span> show that in the future, the use of an AOS with a Rayleigh LGS at this telescope will improve the quality of the formed image by an order of magnitude.</p>","PeriodicalId":478,"journal":{"name":"Astrophysical Bulletin","volume":"80 2","pages":"328 - 336"},"PeriodicalIF":1.4,"publicationDate":"2025-08-21","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"144888114","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 : 2025-05-26DOI: 10.1134/S1990341324600777
A. F. Kholtygin, A. V. Dodin, I. A. Yakunin
The paper is aimed at studying the variability of the Be star (omega) Ori. We analyzed the optical spectra of the star taken with the 2.5-m SAI25 telescope of the Caucasus Mountain Observatory (CMO) of SAI MSU. A rapid variability of the H and He line profiles with periods from 37 to 150 minutes are revealed. The photometric light curves of (omega) Ori obtained with the TESS satellite regular brightness variations with periods of 0.94 and 1.86 days have been detected. We also discuss X-ray observations and search for a magnetic field of (omega) Ori.
本文旨在研究Be星(omega) Ori的变异性。我们对该恒星的光谱进行了分析,该光谱是由SAI MSU高加索山天文台(CMO)的2.5 m SAI25望远镜拍摄的。H线和He线剖面在37 ~ 150分钟的周期内具有快速变率。利用TESS卫星获得了(omega) Ori的光度曲线,其亮度变化周期分别为0.94和1.86 d。我们还讨论了x射线观测和寻找(omega) Ori磁场。
{"title":"Optical and X-Ray Variability of Be Stars: (omega) Ori","authors":"A. F. Kholtygin, A. V. Dodin, I. A. Yakunin","doi":"10.1134/S1990341324600777","DOIUrl":"10.1134/S1990341324600777","url":null,"abstract":"<p>The paper is aimed at studying the variability of the Be star <span>(omega)</span> Ori. We analyzed the optical spectra of the star taken with the 2.5-m SAI25 telescope of the Caucasus Mountain Observatory (CMO) of SAI MSU. A rapid variability of the H and He line profiles with periods from 37 to 150 minutes are revealed. The photometric light curves of <span>(omega)</span> Ori obtained with the TESS satellite regular brightness variations with periods of 0.94 and 1.86 days have been detected. We also discuss X-ray observations and search for a magnetic field of <span>(omega)</span> Ori.</p>","PeriodicalId":478,"journal":{"name":"Astrophysical Bulletin","volume":"80 1","pages":"49 - 57"},"PeriodicalIF":1.3,"publicationDate":"2025-05-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"144140177","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}