类星体和Abell星系团的角相关函数

本文采用目前样品数最大的Hewitt Burbidge类星体总表与覆盖全天区的Abell星系团表 (即ACO表 )研究了类星体与星系团分布的成协问题 .利用交叉相关函数方法 ,发现在角距离θ >3°范围内类星体与Abell团呈反相关现象 .这种反相关主要是由光学选类星体产生的 ,射电选类星体的分布与Abell团基本无关 ,这一事实支持了星系团中尘埃的吸收效应的解释 .在θ <3°范围反而无明显的反相关性 ,说明类星体与星系团存在着成协的倾向 .进一步分析表明类星体与星系团的相关性与红移无关 ,这不利于引力透镜效应的解释     

Virgo星系团中星系与类星体成协

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。     

Virgo星系团中星系与类星体成协

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。     

引力透镜与类星体─星系(星系团)成协

综述了背景光源（类星体）与前方天体（星系、星系团等）成协的观测和统计事例．详尽叙述了与成协问题相关的引力透镜理论．全面介绍了对各种成协事例进行引力透镜理论解释的方法、研究现状及存在的问题．还给出了一种计算成协样品中面密度超出因子的改进方法．     

利用数值模拟方法对类星体-星系团引力透镜成因的再考察

利用星系团形成的数值模拟技术所得到的星系团以及大尺度结构,本文研究了星系团和其周围环境物质的引力透镜效应对背景类星体计数的影响,以期解释最近观测到的类星体星系团成协现象．然而,得到的结果却是：用星系团及所遵循的大尺度结构的引力透镜效应,不能解释所观测到的类星体数密度．这与解析方法所得结论一致．分析表明：目前所观测到的类星体与星系团成协,如果不是统计涨落,则无法用引力透镜效应来解释。     

利用数值模拟方法对类星体—星系团引力透镜成因的再考察

利用星系团形成的数值模拟技术所得到的星系团以及大尺度结构,本研究了星系团的其周围环境物质的引力透镜效应对背景类星体计数的影响,以期解释最近观测到的类星体－星系团成协现象,然而,得到的结果却是：用星系团及所遵循的大尺度结构的引力透镜效应,不能解释所观测的类星体数密度,这与解析方法所得结论一致,分析表明,目前所观测到的类星体与星第团成协,如果不是统计涨落,则无法用引力透镜效应来解释。     

引力透镜与类星体——星系（星系团）成协

综述了背景光源（类星体）与前方天体（星系、星系团等）成协的观测和统计事例。详尽叙述了与成协问题相关的引力透镜理论。全面介绍了对各种成协事例进行引力透镜理论解释的方法、研究现状及存在的问题。还给出了一种计算成协样品中面密度超出因子的改进方法。     

类星体与Uppsala星系位置相关性的统计分析

我们利用最新的类星体星表和Uppsala星系表的资料,对于类星体与星系的成协问题进行了进一步的统计分析。两点交叉相关函数统计方法的结果表明,相对于类星体在天球上完全随机分布而言,平均说来在每一个类星体附近10.0范围内星系数目大约超出0.153±0.011个。同时有迹象表明,随着类星体的红移值或视星等数值的增大,这种成协现象也趋于加强。此外,最邻近间距试验也进一步支持了类星体与星系成协的统计结果。     

与发射线区成协的类星体CIV吸收系统研究（Ⅱ）统计研究（2）

本文是系列文单ＩＩ的第２篇，根据前文的统计结果，我们确认了成协吸收系统的存在，本文在此基础上，对成协吸收系统出现频率与类星体红移，光学亮度，Ｘ射线波段和红外波段辐射性质的相关性进行了讨论，结果表明成协吸收系统与类星体Ｘ射线波段性质无关，而与类星体的红移和光学亮度有关，表现为低红移低光度的类星体中成协系统的出现频率明显地比其它样本高得多。     

类星体的空间分布和与星系成协的统计研究及其演化意义

本文采用了三组具有代表性的类星体观测资料:(1)类星体第二总表,(2)赤纬-40°天区类星体,(3)室女座星系团区类星体。分析的内容包括:类星体红移和星等的大尺度分布,类星体在局部天区内的空间分布,类星体与场星系以及与星系团中亮星系的成协性。 得到的初步结果是:(1)类星体就整体来说其红移和星等在各种尺度上的分布是不均匀的;(2)在局部天区内这种不均匀性表现得更为显著;(3)类星体与场星系的普遍成协性不明显;(4)类星体与星系团中亮星系普遍成协的可能性是统计显著的;(5)类星体在演化上应该具有不同的起源。就其本质来说很可能是宇宙论性和非宇宙论性两者兼之。     

Acceleration of Numerical Integration of the Equations of Motion of Asteroids

Solar System Research - Finding and studying possible collisions of asteroids approaching the Earth requires a significant amount of computation. This paper describes the R0 program created to...     

Equation of state and anisotropy of pressure of magnetars

Magnetars are the neutron stars with the highest magnetic fields up to 10¹⁵–10¹⁶ G. It has been proposed that they are also responsible for a variety of extra-galactic phenomena, ranging from giant flares in nearby galaxies to fast radio bursts. Utilizing a relativistic mean field model and a variable magnetic field configuration, we investigate the effects of strong magnetic fields on the equation of state and anisotropy of pressure of magnetars. It is found that the mass and radius of low-mass magnetars are weakly enhanced under the action of the strong magnetic field, and the anisotropy of pressure can be ignored. Unlike other previous investigations, the magnetic field is unable to violate the mass limit of the neutron stars.     

Observations of the intensity of the penumbra of sunspots

Observations of the penumbral intensity of sunspots in 13 wavelength regions are presented. In 4 wavelength regions 54 sunspots are measured. In the other wavelength regions the number of sunspots considered ranges from 3–19.The penumbral intensity alters with position within the spot. This intensity variation is found to be comparable with the change in intensity from one spot to another. The penumbral intensity is found to be independent of spot size in the sample considered.The penumbra model of Kjeldseth Moe and Maltby (1969) with = 0.055 is supported by the measurements.     

A survey of orbits of co-orbitals of Mars

Many asteroids with a semimajor axis close to that of Mars have been discovered in the last several years. Potentially some of these could be in 1:1 resonance with Mars, much as are the classic Trojan asteroids with Jupiter, and its lesser-known horseshoe companions with Earth. In the 1990s, two Trojan companions of Mars, 5261 Eureka and 1998 VF₃₁, were discovered, librating about the L₅ Lagrange point, 60° behind Mars in its orbit. Although several other potential Mars Trojans have been identified, our orbital calculations show only one other known asteroid, 1999 UJ₇, to be a Trojan, associated with the L₄ Lagrange point, 60° ahead of Mars in its orbit. We further find that asteroid 36017 (1999 ND₄₃) is a horseshoe librator, alternating with periods of Trojan motion. This asteroid makes repeated close approaches to Earth and has a chaotic orbit whose behavior can be confidently predicted for less than 3000 years. We identify two objects, 2001 HW₁₅ and 2000 TG₂, within the resonant region capable of undergoing what we designate “circulation transition”, in which objects can pass between circulation outside the orbit of Mars and circulation inside it, or vice versa. The eccentricity of the orbit of Mars appears to play an important role in circulation transition and in horseshoe motion. Based on the orbits and on spectroscopic data, the Trojan asteroids of Mars may be primordial bodies, while some co-orbital bodies may be in a temporary state of motion.     

Graphical representation of periodic motion of the line of nodes of the Moon

In the text-books of astronomy, sections generally related to the Moon deal with the orbital elements of the Earth-Moon system such asa, e, i, , and the time of perigee passage. While the MEAN of the first of the three elements do not vary, mean longitude of the ascending node-mean longitude of the lunar perigee and the time of perigee passage undergoes secular as well as periodic changes due predominantly to the action of the Sun's gravitational attraction. While to a certain degree, explanations related to the calculation of the lunar orbit parameters are given, not a single graphical representation of these short- or long-periodic changes are presented. We allow the number of data related to these periodic changes must cover a large span of time; and if regression of the line of nodes or advances of the line of apses are to be graphically seen, data covering 18.61 and 8.85 yr, respectively, are needed. In this work we particularly aim at the graphical representation of the periodic changes of the line of nodes.