BL Lac天体ON231的CCD测光积分时间与测光误差分析

积分时间对CCD测光结果的误差有很大影响.利用云南天文台1 m望远镜对BLLac天体ON231进行了I波段不同积分时间的观测,获得了I波段BL Lac天体ON231 CCD测光积分时间与测光误差的关系.结果表明,当BL Lac天体ON231处于低态时,在I波段的最佳积分时间约为294 s,此时测光误差最小.     

施密特望远镜CCD BVRI测光系统的初步研究

本文利用Thomson CCD,在北京天文台兴隆站施密特望远镜上进行BVRI四色测光,得到了该测光系统的颜色转换方程,并对所得结果进行了分析探讨。同时论证了BAO-CCD系统在施密特望远镜上用于测光的可行性。     

兴隆60cm望远镜主焦CCD系统测光性能的研究

对兴隆６０ｃｍ望远镜主焦ＣＣＤ系统的测光性能进行了测试和研究,测定了ＣＣＤ快门时间函数,讨论了快门延迟效应对短时间曝光观测的可能影响,通过观测大批Ｌａｎｄｏｌｔ标准星,较准确地定出了ＢＶＲＩ宽带测光的星等系统转换关系,结果表明本系统与标准ＢＶＲＩ系统很接近,对ＣＣＤ系统的天文测光精度作了仔细的检验和分析,工对ＰＳＦ拟合测光和孔径测光两种方法进行了比较。     

电荷守恒与CCD孔径测光

Lick天文台的CCD控制器是一类新型控制器,它能够在同一CCD系统内实现MPP(Multi—pinned phase)和通常工作模式间的转换．自2002年起中国至少有4架 CCD照相机使用这类控制器．此控制器的弱点是溢出发生在非线性前,而且远在饱和以前．虽然这对亮的面光源观测不利,并且它妨碍了使用亮星构建点扩散函数(psf)．但是由于电荷守恒原理,对亮的点源(恒星)的孔径测光依然可行．观测证明了此结论．     

兴隆60cm反射镜主焦CCD测光系统的基本性能测试

给出兴隆60cm反射镜主焦CCD系统测光性能的测试结果，内容包括bias和暗流的稳定性测试、平场分析、增益和读出噪声测定等。以期为CCD测光工作提供参考和指导。     

CCD图像相对测光中的技术研究与精度回报现象

天体随时间的光度变化能够反映其物理性质,高精度测光技术有助于我们更好地分析与探究天体的光变情况,对天体的演化研究有重要意义.介绍了相关的测光工具与技术,探索了把MaxIm DL与photutils测光库相结合的测光技术及应用,提出了连续图像中各星像测光数据快速匹配的解决方案.通过分析中国科学院云南天文台1m光学望远镜拍...     

CCD照相测量天荒坪大气消光系数实验（二）：测光篇

“大气消光”是天文观测中不可回避的基础性问题,在以往的天文奥赛中曾多次作为考点（例如2006年IAO）。本文对此进行了相当详细的调研和实测,并撰写了本文和同好们分享。对高年组选手而言,这是一份有价值的参考资料：低年组选手只需记住基本概念即可,对文中的难点不必过于深究。     

兴隆60 cm望远镜主焦CCD系统测光性能的研究

对兴隆６０ｃｍ望远镜主焦ＣＣＤ系统的测光性能进行了测试和研究．测定了ＣＣＤ快门时间函数,讨论了快门延迟效应对短时间曝光观测的可能影响．通过观测大批Ｌａｎｄｏｌｔ标准星,较准确地定出了ＢＶＲＩ宽带测光的星等系统转换关系,结果表明本系统与标准ＢＶＲＩ系统很接近．对ＣＣＤ系统的天文测光精度作了仔细的检验和分析,并对ＰＳＦ拟合测光和孔径测光两种方法进行了比较     

关于CCD平场快门效应的改正及有关问题

本文对文献中报道的两种测定快门效应改正的方法进行了讨论．我们指出，对反光镜卡焦，即使面光源本身亮度分布均匀，照射在ＣＣＤ上的辐射也可以不均匀，允许有一个二维分布。但如果这种亮度的相对分布在晨昏蒙影过程中也变化，则Ｓｕｒｍａ方法的应用便要受到影响，而这是许多人忽略的．从单纯测定快门改正函数的角度看，圆顶平场法测定更简单准确．可惜，大多数情况下精确改正快门效应的目的是同时得到精确的平场．如果要求１％或更高精度的平场，单测定快门改正还不够．对每架给定的反光镜，如何测定平场本身都是需要仔细研究的事． 作为例子，给出了佘山１．５６米反光镜加Ｔｈｏｍｓｏｎ ＲＣＣＤ（１０２４ ｘ １０２４像元）的快门改正测定．     

关于云南天文台Tek 1024CCD的线性及其他

云南天文台新安装的Tek 1 0 2 4× 1 0 2 4CCD系统是一个很好的系统。天文上应用CCD的主要目的是测量暗弱天体 ,该系统满足这个要求。但在亮端 ,测量显示 ,当读数大于 2万多adu时 ,CCD响应对线性的偏离已经开始大于 1 % ,当读数接近 6 0 0 0 0adu时 ,响应不但是非线性的 ,而且显得不稳定。另外 ,顺便给出用 1 0 0KHz读出的bias图并作了讨论     

窄线赛弗特1星系Arakelian564的测光

使用上海天文台 1.5 6m望远镜 ,对窄线赛弗特 1星系Ark 5 6 4进行了时间跨度为 3星期的观测 ,给出了VRI波段的光学观测结果。使用交叉相关方法研究了三个波段之间的时间延迟 ,但是未发现有时间延迟     

Gain calibration of CCD systems at VBO

The system gain of two CCD systems in regular use at the Vainu Bappu Observatory, Kavalur, is determined at a few gain settings. The procedure used for the determination of system gain and base-level noise is described in detail. The Photometrics CCD system at the 1-m reflector uses a Thomson-CSF TH 7882 CDA chip coated for increased ultraviolet sensitivity. The gain is programme-selected through the parameter ‘cgain’ varying between 0 and 4095 in steps of 1. The inverse system gain for this system varies almost linearly from 27.7 electrons DN^-1 at cgain = 0 to 1.5 electrons DN^-1 at cgain = 500. The readout noise is ≲ 11 electrons at cgain = 66. The Astromed CCD system at 2.3-m Vainu Bappu Telescope uses a GEC P8603 chip which is also coated for enhanced ultraviolet sensitivity. The amplifier gain is selected in discrete steps using switches in the controller. The inverse system gain is 4.15 electrons DN^-1 at the gain setting of 9.2, and the readout noise ∼ 8 electrons.     

NAOC 1m反射望远镜CCD相机的性能研究

研究了国家天文台兴隆观测基地1m反射望远镜新安装的VersArray1340×1300BCCD照相机的性能。它有几乎没有图案的良好本底（bias），极低的读出噪声和暗流。用平场序列露光来检测其线性时，能得到线性良好的转移曲线（transfercurve）。但是，不论在平场露光（面光源）还是在恒星（点光源）的观测中，当像元值约高于55000adu时（增益3．7e^-／adu），都会产生溢出。此时CCD并未满井。因此，使用它做点扩散函数分析研究时，要避免使用太亮的星像。不过，由于电荷守恒原理，对产生溢出的孤立亮星像，仍然可以做孔径测光。此外，该相机的快门函数也已测定。     

CCD star images: On the determination of Moffat’s PSF shape parameters

Among the variety of empirical models of optical Point Spread Function used in the astronomical environment, only the Moffat’s (1969) one is able to describe by means of two parameters (in the circular case) both the inner and the outer star image regions. In view of this very important feature, the problem of the simultaneous estimates of Moffat’s PSF shape parameters, off-centring, and the background level in CCD star images has been investigated. The problem does not seem to be rigorously resolvable, but an approximate way to calculate all the parameters except off-centring is shown. It must be stressed that, the Moffat’s PSF model being a softened power law belonging to the family of modified King and Hubble models, the present discussion can be of aid in many other research fields. Also, the integral equation enabling us to convolve a spherical source with Moffat’s PSF is given and applied for comparison to Multi-Gaussian convolution.     

CCD Photometry of Asteroids 38, 174, 276 and 346

Photometric observations of the four selected asteroids, obtained at Yunnan Observatory, China during recent two years, are presented and analysed. We have determined the synodic periods of (174)\, Phaedra and (276)\, Adeldheid as 5.74h ± 0.01 and 6.29h ± 0.01,which confirmed the previous results. For (38)\, Leda and (346)\, Hermentria, we derived their period values, 10.171h ± 0.007 and 19.408h ± 0.005 for the first time. The color-indices of 38, were re-determined as 0.73 ± 0.02 for B-V and 0.41 ± 0.02for U-B, respectively, which are the same as the ones given by Tedesco (1989).     

云南天文台1米反光镜CCD系统的性能补充

云南天文台新安装的Tek 1024×1024 CCD照相机性能良好,本文讨论了该CCD使用手册上没有列出的某些性能,包括:bias的pattern;oversacn区;坏象元问题;以及快门效应。     

CCD photometry of RV rau stars. VII. EP lyrae

Photometric observations of the variable star EP Lyr were performed with a CCD photometer during the observing season of 2002. Analysis of these observations together with published data has confirmed the mean period of the main variability cycle P = 83.^d248 over almost 100 years. The periodicity of the variations in the main cycle is investigated on the basis of O-C diagrams. The time scale of its variations ranges from 1–2 to 8–20 thousand days.     

CCD photometry of RV tau stars. VI. TX ophiuchii

Photometric observations of the variable star TX Oph were performed with CCD photometers during the observing seasons of 1999, 2000, and 2002. Analysis of these observations together with published data has confirmed the mean period of the main variability cycle P = 135^d. 2613 over almost 70 years. A secondary cycle with a period of about 10–12 thousand days has also been found.