In this paper we explore the formation of bars and present the bulge and bar properties and their correlations for a sample of lenticular barred(SB0)and lenticular unbarred(S0)galaxies in the central region of the Com...In this paper we explore the formation of bars and present the bulge and bar properties and their correlations for a sample of lenticular barred(SB0)and lenticular unbarred(S0)galaxies in the central region of the Coma Cluster using HST/ACS data.In our sample,we identified bar features using the luminosity profile decomposition software GALFIT.We classified the bulges based on Sérsic index and Kormendy relation.We found that the average mass of the bulge in SB0 galaxies is 1.48×10^(10)M☉whereas the average mass of the bulge in S0 galaxies is 4.3×10^(10)M☉.We observe that SB0 galaxies show lower bulge concentration,low mass and also smaller B/T values compared to S0 galaxies.Using the Kormendy relation,we found that among the lenticular barred galaxies,82%have classical bulges and 18%have pseudo bulges.These classical bulges have low masses compared to the classical bulges of unbarred galaxies.S0,galaxies with massive classical bulges do not host bars.We also found that for all SB0s the bulge effective radius is less than the bar effective radius.SB0 galaxies with classical bulges suggest that the bar may have formed by mergers.展开更多
This paper presents a preliminary test of the k-th nearest neighbor distance （KNND） method for detecting nearby open clusters based on Gaia-DR1. We select 38 386 nearby stars （〈 100 pc） from the Gaia-DR1 catalog,...This paper presents a preliminary test of the k-th nearest neighbor distance （KNND） method for detecting nearby open clusters based on Gaia-DR1. We select 38 386 nearby stars （〈 100 pc） from the Gaia-DR1 catalog, and then use the KNND method to detect overdense regions in three-dimensional space. We find two overdense regions （the Hyades and Coma Berenices （Coma Ber） open clusters）, and obtain 57 reliable cluster members. Based on these cluster members, the distances to the Hyades and Coma Ber clusters are determined to be 46.0±0.2 and 83.5±0.3 pc, respectively. Our results demonstrate that the KNND method can be used to detect open clusters based on a large volume of astrometry data.展开更多
基于Gaia Data Release 2 (Gaia-DR2)星表,采用数据挖掘技术中的DBSCAN(Density-Based Spatial Clustering of Applications with Noise)算法进行邻近疏散星团成员检测.从Gaia-DR2中选取了594284颗恒星(距离太阳<100 pc)作为样本,使...基于Gaia Data Release 2 (Gaia-DR2)星表,采用数据挖掘技术中的DBSCAN(Density-Based Spatial Clustering of Applications with Noise)算法进行邻近疏散星团成员检测.从Gaia-DR2中选取了594284颗恒星(距离太阳<100 pc)作为样本,使用恒星的五维数据(三维空间位置和两维自行)进行聚类分析.在数据预处理阶段,将每一维数据标准化到[0, 1]区间内,避免了单位不一致对聚类效果的影响.然后,利用k-dist图确定了DBSCAN算法的输入参数(Eps, MinPts).最终,使用DBSCAN算法获取了133颗成员星,它们在五维相空间中可以被分成两组,分别对应于疏散星团Hyades和Coma.分析结果表明得到的成员星是可靠的.根据两个星团的成员星, Hyades和Coma的距离分别确定为(46.5±0.3) pc和(84.9±0.4) pc.展开更多
A cosmological model was developed using the equation of state of photon gas, as well as cosmic time. The primary objective of this model is to see if determining the observed rotation speed of galactic matter is poss...A cosmological model was developed using the equation of state of photon gas, as well as cosmic time. The primary objective of this model is to see if determining the observed rotation speed of galactic matter is possible, without using dark matter (halo) as a parameter. To do so, a numerical application of the evolution of variables in accordance with cosmic time and a new state equation was developed to determine precise, realistic values for a number of cosmological parameters, such as energy of the universe <i>U</i>, cosmological constant <i>E</i><sub>Λ</sub>, curvature of space <i>k</i>, energy density <i>ρ</i><sub>Λ<i>e</i></sub>, age of the universe <i>t</i><sub>Ω</sub> (part 1). That energy of the universe, when taken into consideration during the formation of the first galaxies (<1 [Gy]), provides a relatively adequate explanation of the non-Keplerian rotation of galactic masses (part 2). Indeed, such residual, non-baryonic energy, when considered in Newton’s gravity equation, adds the term <i>F</i><sub>Λ</sub>(<i>r</i>), which can partially explain, without recourse to dark matter, the rotations of some galaxies, such as M33, UGC12591, UGC2885, NGC3198, NGC253, DDO161, UDG44, the MW and the Coma cluster. Today, in the MW, that cosmological gravity force is in the order of 10<sup>26</sup> times smaller than the conventional gravity force. The model predicts an acceleration of the mass in the universe (<i>q</i>~-0.986);the energy associated with curvature <i>E<sub>k</sub></i> is the driving force behind the expansion of the universe, rather than the energy associated with the cosmological constant <i>E</i><sub>Λ</sub>. An equation to determine expansion is obtained using the energy form of the Friedmann equation relative to Planck power <i>P<sub>P</sub></i> and cosmic time or Planck force <i>F<sub>P</sub></i> acting at the frontier of the universe moving at <i>c</i>. This constant Planck force, from unknown sources, acts everywhere to the expansion of the universe as a stretching effect on the volume. Finally, the model partly explains the value a<sub>0</sub> of the MOND theory. Indeed, <i>a</i><sub>0</sub> is not a true constant, but depends on the cosmological constant at the time the great structures were formed (~1 [Gy]), as well as an adjustment of the typical mass and dimension of those great structures, such as galaxies. The constant a<sub>0</sub> is a different expression of the cosmological gravity force <i>F</i><sub>Λ</sub> as expressed by the cosmological constant, Λ, acting through the energy-mass equivalent during the formation of the structures. It does not put in question the value of <i>G</i>.展开更多
文摘In this paper we explore the formation of bars and present the bulge and bar properties and their correlations for a sample of lenticular barred(SB0)and lenticular unbarred(S0)galaxies in the central region of the Coma Cluster using HST/ACS data.In our sample,we identified bar features using the luminosity profile decomposition software GALFIT.We classified the bulges based on Sérsic index and Kormendy relation.We found that the average mass of the bulge in SB0 galaxies is 1.48×10^(10)M☉whereas the average mass of the bulge in S0 galaxies is 4.3×10^(10)M☉.We observe that SB0 galaxies show lower bulge concentration,low mass and also smaller B/T values compared to S0 galaxies.Using the Kormendy relation,we found that among the lenticular barred galaxies,82%have classical bulges and 18%have pseudo bulges.These classical bulges have low masses compared to the classical bulges of unbarred galaxies.S0,galaxies with massive classical bulges do not host bars.We also found that for all SB0s the bulge effective radius is less than the bar effective radius.SB0 galaxies with classical bulges suggest that the bar may have formed by mergers.
基金supported by the National Natural Science Foundation of China(NSFC,Grant No.11403004)
文摘This paper presents a preliminary test of the k-th nearest neighbor distance （KNND） method for detecting nearby open clusters based on Gaia-DR1. We select 38 386 nearby stars （〈 100 pc） from the Gaia-DR1 catalog, and then use the KNND method to detect overdense regions in three-dimensional space. We find two overdense regions （the Hyades and Coma Berenices （Coma Ber） open clusters）, and obtain 57 reliable cluster members. Based on these cluster members, the distances to the Hyades and Coma Ber clusters are determined to be 46.0±0.2 and 83.5±0.3 pc, respectively. Our results demonstrate that the KNND method can be used to detect open clusters based on a large volume of astrometry data.
文摘A cosmological model was developed using the equation of state of photon gas, as well as cosmic time. The primary objective of this model is to see if determining the observed rotation speed of galactic matter is possible, without using dark matter (halo) as a parameter. To do so, a numerical application of the evolution of variables in accordance with cosmic time and a new state equation was developed to determine precise, realistic values for a number of cosmological parameters, such as energy of the universe <i>U</i>, cosmological constant <i>E</i><sub>Λ</sub>, curvature of space <i>k</i>, energy density <i>ρ</i><sub>Λ<i>e</i></sub>, age of the universe <i>t</i><sub>Ω</sub> (part 1). That energy of the universe, when taken into consideration during the formation of the first galaxies (<1 [Gy]), provides a relatively adequate explanation of the non-Keplerian rotation of galactic masses (part 2). Indeed, such residual, non-baryonic energy, when considered in Newton’s gravity equation, adds the term <i>F</i><sub>Λ</sub>(<i>r</i>), which can partially explain, without recourse to dark matter, the rotations of some galaxies, such as M33, UGC12591, UGC2885, NGC3198, NGC253, DDO161, UDG44, the MW and the Coma cluster. Today, in the MW, that cosmological gravity force is in the order of 10<sup>26</sup> times smaller than the conventional gravity force. The model predicts an acceleration of the mass in the universe (<i>q</i>~-0.986);the energy associated with curvature <i>E<sub>k</sub></i> is the driving force behind the expansion of the universe, rather than the energy associated with the cosmological constant <i>E</i><sub>Λ</sub>. An equation to determine expansion is obtained using the energy form of the Friedmann equation relative to Planck power <i>P<sub>P</sub></i> and cosmic time or Planck force <i>F<sub>P</sub></i> acting at the frontier of the universe moving at <i>c</i>. This constant Planck force, from unknown sources, acts everywhere to the expansion of the universe as a stretching effect on the volume. Finally, the model partly explains the value a<sub>0</sub> of the MOND theory. Indeed, <i>a</i><sub>0</sub> is not a true constant, but depends on the cosmological constant at the time the great structures were formed (~1 [Gy]), as well as an adjustment of the typical mass and dimension of those great structures, such as galaxies. The constant a<sub>0</sub> is a different expression of the cosmological gravity force <i>F</i><sub>Λ</sub> as expressed by the cosmological constant, Λ, acting through the energy-mass equivalent during the formation of the structures. It does not put in question the value of <i>G</i>.
