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1.
在小波分析的基础上,用峰值计数法考察了Virgo团天区的结构与次结构。在Virgo团典型的双峰结构下面,发现还有180’和120‘两个明显的次结构的特征尺度,该结果有力地支持了等级式的成团模式。与之对应的波长下的小波强度分布清楚地显示了Virgo团丰富的次结构及其分布情况,从中还发现了两个新的较小的次结构。  相似文献   

2.
本文对Virgo星系团中央6°天区内的成员星系作了光度函数和质量函数的研究。成员星系是以视向速度作为判据并合理地考虑了密度分布因素后确定的。研究表明,该天区全部成员星系的光度函数为Schechter型,而各类S星系的光度函数则为Gauss型,且峰值位置按Sa→Sd序列向暗端移动,宽度亦逐渐变宽;Virgo团质量函数与恒星质量函数一样可以用指数形式来描述,文中还利用光度函数和质量函数对该团的形态和质量分层进行了讨论,并计算了该天区团的总光度。  相似文献   

3.
根据LBQS在Virgo天区的类星体样品和BST的Virgo星系团的星系样品,利用交叉相关函数的方法研究了类星体与星系成协的现象,发现在角间距5'<θ<40'范围内成员星系与类星体有明显的成协性。而对背景星系不存在这种成协现象。本文还讨论了成协与视星等的关系问题。  相似文献   

4.
根据LBQS在Virgo天区的类星体样品和BST的Virgo星系团的星系样品,利用交叉相关函数的方法研究了类星体与星系成协的现象,发现在角间距5'<θ<40'范围内成员星系与类星体有明显的成协性。而对背景星系不存在这种成协现象。本还讨论了成协与视星等的关系问题。  相似文献   

5.
利用基于自校正和CLEAN算法的现代VLBI混合成图技术,对Pearson等人于1976年观测得到的类星体 3C 286在 18 cm波段上的 VLBI数据重新作了处理.由此得到的图像要大大好于最初的处理结果,也获得了更多的有用信息.用几个Gauss模型去拟合校正后的UV数据,发现中央亮区可以被分解为两个致密结构,这与后来的高分辨率观测相一致.与不同历元的VLBI观测结果相比较,发现这两个致密结构间的距离不但在同一时间随观测频率变化,而且很有可能在同一观测频率上随时间变化.  相似文献   

6.
本文报道南天区5GHzVLBI的第二轮观测.第二轮观测是在1993年5月期间进行的,共观测了25个射电源,检测到24个源,获得了23个南天区耀变体(Blazar)的VLBI高分辨率的图象,其中15个是第一次VLBI成图,7个是高能(>100MeV)γ射电源,12个源呈现核-喷流结构,其余11个源是单一的致密核,未发现致密双源.有两个源可能有视超光速现象.  相似文献   

7.
在1991—1993年期间,Comptonγ射线天文台(CGRO)在射电源PKS0528+134中观测到两次很强的射线爆发,都伴随有毫米波射电大爆发.本文详细分析了高能γ-X射线波段和红外-光学波段的辐射能量分布(SED).结果表明,高能γ射线辐射可能主要是由喷流相对论电子对周围UV-软X射线光子的逆康普顿散射所产生的.同时,通过毫米波射电大爆发的频谱演化特性与γ射线源的同步辐射频谱特性的比较,对γ辐射等离子团和射电等离子团之间可能的演化联系作了讨论.  相似文献   

8.
本文利用在考虑团内星系面数密度分布的前提下,以视向速度为判据,按最大似然原理解算团分布参数和成员概率的严格统计方法,对8个Abell星系团进行了成员研究.解算结果表明此方法是合理的、有效的,星系团的速度弥散度分布与动力学模型一致.有迹象表明椭长形的结构在星系团中是一种普遍现象.从这8个团得到了清晰的NA-σc的相关关系,进而推知团的质光比为100~600h,平均350h.  相似文献   

9.
研究了海尔-波普彗星1996年9月的光变曲线,发现其在9月10日至11日发生了一次爆发,爆发时核V星等增亮2.1m.相应地,在CCD图像上也发现爆发时彗核抛出的2个球状凝聚物.  相似文献   

10.
本文利用确定的278个视向速度成员星系,讨论了Coma星系团的结构和中心区的次团结构.分析表明,Coma团内星系表现有一定程度的空间形态分层和质量分层,早型星系同晚型星系相比,大质量星系与较小质量星系相比,前者的面分布明显地有向团中心集聚的倾向.按最大似然原理对星系的视向速度的分析表明,Coma团中心区可能存在着次团结构.  相似文献   

11.
In this paper, we present a “peak number count method”, based on wavelet transformation, and use it to explore the structure and substructures in the Virgo area. It is found that, besides the two-humped structure, there are also quite a lot of small subclusters with characteristic scales of 180′ and 120′. This result strongly supports the hierarchical clustering model of structures. The wavelet coefficient map clearly shows these substructures and their distributions. Additionally, two new small subclusters are discovered.  相似文献   

12.
The 'algorithm driven by the density estimate for the identification of clusters' ( DEDICA ) is applied to the A3558 cluster complex in order to find substructures. This complex, located at the centre of the Shapley Concentration supercluster, is a chain formed by the ACO clusters A3556, A3558 and A3562 and the two poor clusters SC 1327-312 and SC 1329-313. We find a large number of clumps, indicating that strong dynamical processes are active. In particular, it is necessary to use a fully three-dimensional sample (i.e. using the galaxy velocity as third coordinate) in order also to recover the clumps superimposed along the line of sight. Even though a large number of detected substructures was already found in a previous analysis, this method is more efficient and faster when compared with a wide battery of tests, and permits the direct estimate of the detection significance. Almost all subclusters previously detected by the wavelet analyses found in the literature are recognized by DEDICA . On the basis of the substructure analysis, we also briefly discuss the origin of the A3558 complex by comparing two hypotheses: (i) the structure is a cluster–cluster collision seen just after the first core–core encounter; or (ii) this complex is the result of a series of incoherent group–group and cluster–group mergings, focused in that region by the presence of the surrounding supercluster. We studied the fraction of blue galaxies in the detected substructures and found that the bluest groups reside between A3562 and A3558, i.e. in the expected position for the scenario of cluster–cluster collision.  相似文献   

13.
We use numerical N -body simulations of the Orion Nebula Cluster (ONC) to investigate the possibility of substructure in its formation. There is no substructure apparent in the ONC today. However, unless there was a remarkable degree of homogeneity in the molecular cloud from which it formed, it seems unlikely that this would have been true of the cluster in its earliest phase. More plausibly, the early structure of the cluster would have consisted of groups or clumps of subclusters, following the structure of the cloud itself. We have explored the extent to which such subclusters could subsequently have merged, and find that the age of the cluster is a critical factor. The most inhomogeneous initial conditions, comprising a small number of subclusters with many members, are ruled out by an age of 2 Myr or less. There is a considerable amount of freedom in the other direction, however, which suggests that fragmentation in the original cloud is more likely to have been on the scale of small clumps, each producing fewer than 100 stars. These initial subclusters could have been very dense – perhaps two or three orders of magnitude more dense than the core of the ONC today.  相似文献   

14.
在GPS数据处理中 ,存在着误差影响、影响波的干扰、周跳和数据量大等问题。误差影响和影响波的干扰实质是在接收卫星信号时受到其它因素的影响 ;周跳是由于卫星信号的失锁而造成信号的不连续 ;数据量大是因为GPS观测需要采样间隔小又连续观测所致。由于小波理论具有时频分析、波形分解、特征提取和快速小波变换等特性 ,应用小波变换和波形分解可以解决误差影响和影响波的干扰的问题 ;应用特征提取可以解决周跳检测问题 ;应用快速小波变换可进行数据压缩  相似文献   

15.
A significant fraction of clusters of galaxies are observed to have substructure, which implies that merging between clusters and subclusters is a rather common physical process in cluster formation. It still remains unclear how cluster merging affects the evolution of cluster member galaxies. We report the results of numerical simulations that show the dynamical evolution of a gas-rich, late-type spiral in a merger between a small group of galaxies and a cluster. The simulations demonstrate that the time-dependent tidal gravitational field during merging excites non-axisymmetric structure of the galaxy, subsequently drives efficient transfer of gas to the central region and finally triggers a secondary starburst. This result provides a close physical relationship between the emergence of starburst galaxies and the formation of substructure in clusters. We accordingly interpret post-starburst galaxies located near substructure of the Coma Cluster as one observational example indicating the global tidal effects of group–cluster merging. Our numerical results further suggest a causal link between the observed excess of blue galaxies in distant clusters and the cluster virialization process through hierarchical merging of subclusters. This revised version was published online in July 2006 with corrections to the Cover Date.  相似文献   

16.
Daubechies小波可以表征为幂函数或e指数函数的形式 ,保持相关相位条纹的幅角不变。在VLBI观测信号相关处理过程中引入了小波分析方法 ,以探讨小波理论在VLBI技术中的应用特点。两个台站的VLBI观测信号经过时间补偿和干涉条纹旋转后 ,利用静态小波算法在线性空间中的保角变换特征可提取VLBI信号的干涉相位特征 ,并完整保留相位的时序关系。  相似文献   

17.
We present and discuss a method to identify substructures in combined angular-redshift samples of galaxies within clusters. The method relies on the use of the discrete wavelet transform (hereafter DWT) and has already been applied to the analysis of the Coma cluster. The main new ingredient of our method with respect to previous studies lies in the fact that we make use of a 3D data set rather than a 2D one. We test the method on mock cluster catalogues with spatially localized substructures and on a N -body simulation. Our main conclusion is that our method is able to identify the existing substructures provided that: (a) the subclumps are detached in part or all of the phase space, (b) one has a statistically significant number of redshifts, increasing as the distance decreases due to redshift distortions; (c) one knows a priori the scale on which substructures are to be expected. We have found that to allow an accurate recovery we must have both a significant number of galaxies (≈200 for clusters at z ≥0.4 or about 800 at z ≤0.4) and a limiting magnitude for completeness m B =16.
The only true limitation to our method seems to be the necessity of knowing a priori the scale on which the substructure is to be found. This is an intrinsic drawback of the method and no improvement in numerical codes based on this technique could make up for it.  相似文献   

18.
Six subclusters in the Coma cluster have been selected on the basis of a hierarchical clustering method that takes the gravitational interaction among galaxies into account. Of these, 3 central subclusters around the galaxies NGC 4889, NGC 4874, and NGC 4839 have been singled out. We have used the objective statistical criterion applied by Vennik and Anosova in studies of close groups of galaxies to evaluate each member included in a subcluster with a high probability. Galaxies with a significant deficit of hydrogen HI, including objects from the Bravo-Alfaro list, have been identified with members of the subclusters, with the greatest number of them in the subclusters around NGC 4874 and NGC 4839. A quantitative estimate of the hydrogen deficit using the HI index in the RCG3 catalog reveals a statistically significant excess value for those galaxies that are members of the subclusters compared to galaxies with a hydrogen deficit in the overall Coma cluster field. A substantial number of the spiral galaxies with a hydrogen deficit in the subclusters turned out to be radio galaxies as well. __________ Translated from Astrofizika, Vol. 48, No. 4, pp. 515–528 (November 2005).  相似文献   

19.
对星系团次结构研究中所应用的各种统计学方法进行了全面的评述.内容包括:次结构存在可能性的统计探测、团结构分析以及次团的运动学参数拟合和成员的统计确定.  相似文献   

20.
The quantification of stochastic substructures seen propagating away from the centers of emission lines of Wolf-Rayet (WR) stars is extended using the powerful, objective technique of wavelet analysis. Results for the substructures in one WR star so far show that the scaling laws between (a) flux and velocity dispersion and (b) lifetime and flux, combined with (c) their mass spectrum, strongly support the hypothesis that we are seeing the high mass tail-end distribution of full-scale supersonic compressible turbulence in the winds. This turbulence sets in beyond a critical radius from the star and shows remarkable similarity to the hierarchy of cloudlets seen in giant molecular clouds and other components of the ISM.The velocity dispersion is larger on average for substructures (interpreted as density enhanced turbulent eddies) propagating towards or away from the observer, suggesting that the turbulence is anisotropic. This is not surprising, since the most likely force which drives the windand the ensuing turbulence alike, radiation pressure, is directed outwards in all directions from the star. It is likely that a similar kind of turbulence prevails in the winds of all hot stars, of which those of WR stars are the most extreme.The consequences of clumping in winds are numerous. One of the most important is the necessary reduction in the estimate of the mass-loss rates compared to smooth outflow models.  相似文献   

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