根据数字化巡天光盘测定天体E或V星等

用目视和底片密度扫描的办法从帕洛玛巡天底片得到天体星等资料已有许多作讨论过，其结果得到广泛的应用，考虑到帕洛至于底片已经数字化并做出了数字化巡天光盘（ＤＳＳ），若从它直接得到测光资料将更为方便，为此，我们发展了直接从ＤＳＳ中得到天区天体Ｅ或Ｖ星等的软件，其测量Ｅ星等的精度为０．３７＾ｍ，Ｖ星等的精度为０．４２＾ｍ。     

变星及发射线星系的计算机自动搜索

本文发展了一套计算机自动证认，交叉比对的技术，应用于１９８年９月至１２月间北京天文台６０／９０ｃｍ施密特望远镜的ＣＣＤ测光资料及ＧＳＣ星表，由二个系统的Ｖ星等资料，在６个平方度内找到５颗变星；利用二个系统Ｂ颜色带宽的不同，进行发射线星系统巡天，在３个平方度内找到１５个致密核发射线星秒并讨论了本方法用光变天体，色指数反常天体，位置移动天体，发射线天体巡天的可能性。     

卫星积分多普勒定位观测的初归算结果

本对１９８４年４月－１９８５年４月在南京紫金山山上大人卫测点，用积分多普勒观测的二维单点定位资料进行了分析。并根据卫星来自ＳＥ、ＳＷ、ＮＥ、ＮＷ四个象限获取的资料，分别进行了归算和处理，结果精度如下：σφ（ＳＥ）＝３．７ｍ，σφ（ＳＷ）＝４．２ｍ σφ（ＮＥ）５．１ｍ，σφ（ＮＷ）＝６．５ｍ σλ（ＳＥ）＝４．９ｍ，σλ（ＳＷ）＝５．６ｍ σλ（ＮＥ）３．３ｍ，σλ（ＮＷ）＝４．０ｍ上述表达式中     

CTIO1m反射望远镜的色折射改正和星等差

利用ＣＴＩＯ（ＣｅｒｒｏＴｏｌｏｌｏＩｎｔｅｒ－ＡｍｅｒｉｃａｎＯｂｓｅｒｖａｔｏｒｙ）１ｍ反射望远镜观测球状星团ωＣｅｎ区域的Ｖ和Ｂ波段的照相底片，分析研究了色折射改正；描述了测定色折射改工项系数的方法，得到该望远镜在Ｖ和Ｂ波段照相观测的色折射改正项的系数分别为１．３５２１″和４．５４０３″．随后分析讨论了与星等有关的系统误差，结果表明，对大部分照相压片，星等差是很明显的．在利用底片常数归算时，星等的线性和二次项必须包括在内．     

射电源0716 714和0839 187的光学定位

利用北京天文台具有ＣＣＤ终端的６０ｃｍ光学望远镜（Ｖ波段）观测射电源的光学对应体，得到了０７１６＋７１４和０８３９＋１８７精确的光学位置。参考星表采用拉帕尔玛（ＬａＰａｌｍａ）的１８ｃｍ全自动子午环观测资料编制的ＣＡＭＣ星表，该星表是ＦＫ５星表系统。两颗源位置的内符精度约为０．″１９，与其他作者给出的光学和射电位置观测结果分别进行了比较     

星族综合模型与星系的颜色演化

本文利用Ｂｅｒｔｅｌｉ等人新算出的等龄线，以及Ｇｕｎｎ和Ｓｔｒｙｋｅｒ观测的恒星光谱（３１３０－１０８００）构造了一个星族综合模型．该模型能预计金属丰度在Ｚ＝０．０００４－０．０５，年龄在１０７－２×１０１０年范围内的简单星族（ＳＳＰ）的光谱能量分布（ＳＥＤ）．利用ＳＳＰ，通过对不同时刻恒星形成率的卷积能够得到星系的ＳＥＤ的演化．我们计算出ＳＳＰ以及星系在ＵＢＶＲＩ系统和ＢＡＴＣ１５色中带测光系统中的颜色．计算出的从Ｅ／ＳＯ到Ｓｄｍ各类星系的ＵＢＶＲＩ颜色在年龄为１２Ｇｙｒ时都和观测符合较好．因此，我们的模型为正在进行的关于星系ＳＥＤ的多色测光研究提供了理论上的探索．     

疏散星团M11的研究：1.自行测定与成员研究

本文利用中国科学院上海天文台４０厘米双筒天体照相仪所拍摄得的１０对底片（历元差１６─７０年），经ＰＤＳ测量仪测量，共确定了疏散星团Ｍｌｌ天区８７２颗恒星的相对自行，其中８５％以上恒星的自行测定精度好于±０″．１／百年．利用所测得的相对自行和新的数学模型，确定了不同星等组恒星的分布参数并计算了团中心距ｒ≤２５＇内７８５颗恒星的成员概率，其中成员概率大于０．７的恒星共有５４１颗．详细的讨论表明，新方法不仅在理论上更为严格，实用上也是可行的，可以使星团成员确定取得更为合理的结果．     

由NVSS证认的射电类星体

通过对２０００年版Ｖｅｒｏｎ类星体星表和ＮＶＳＳ巡天数据进行交叉证认,得到了３０１颗新发现有射电辐射的类星体,计算了射电类星体的射电谱指数、射电光度、偏振度等物理量并进行了统计分析,讨论了射电类星体所理比例随红移和绝对星等的分布,以及夺度随红移的演化关系。结果发现,强射电类星体在所有类星体中所占的比例Ｆ（ＲＬＱ）随着ＭＢ的增加而增大,随红移的演化是ｚ＝０．０到ｚ＝０．８逐渐上升,在ｚ＝１．５附近开     

50个发射线天体的物端稜镜光谱

从1981年开始,北京天文台开展了发射线星系的物端稜镜巡天。用60/90cm Schmidt望远镜加5.°3的物端稜镜在敏化的ⅢaJ底片上可以得到亮于16~m的星系光谱像。本文公布了第一批巡天结果:在覆盖天区约220平方度的12张底片上证认出50个发射线天体,47个河外星系(其中3个可能是新的Seyfert星系),3个行星状星云(其中一个N2242以前被当作河外星系)。文中给出了这些天体的名称、坐标、星等及光谱结构分类等资料,并比较系统地讨论了发射线星系的证认及光谱结构分类。我们还将本巡天的结果与其他天文台的结果作了比较。这些天体的证认图见图版Ⅰ—Ⅱ。     

土星卫星CCD定位观测的初步分析

发表了１９９４年８月土星主要卫星ＣＣＤ观测的相对位置资料及其与理论值的比较分析。观测使用了开放实验室分山基地的１５６ｃｍ天体测量望远镜上的ＣＣＤ探测器．对观测资料的分析表明；Ｒｈｅａ和Ｄｉｏｎｅ相对于Ｔｉｔａｎ的位置精度为０．１２”。这相当于距离土星７００ｋｍ．土星卫星ＣＣＤ观测与最佳的照相观测比较，其位置精度相当。     

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...     

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.     

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.