共查询到20条相似文献，搜索用时 156 毫秒
1.
利用国内首个自上向下热蒸发反射膜的大型镀膜机ZZS3200,开展了2.4 m望远镜主镜镀膜工艺的研究。从镀膜的环境控制,镀膜机蒸发源布置,保护膜的选择,旧膜脱膜等方面出发,探索一种适合2.4 m望远镜主镜的镀膜工艺流程,并依此完成2.4 m望远镜主镜镀带MgF2保护的铝反射膜工作。陪镀片检测表明,铝膜膜厚极大极小值差43 nm,主镜反射膜在350~1 100 nm范围内平均反射率87.16%,经2.4 m望远镜实测,镀膜完成后极限星等不低于23.5 mag,比镀膜前约提高1 mag。2013年12月17日,在2.4 m望远镜上,利用终端云南天文台暗弱天体分光及成像仪(Yunnan Faint-Object Spectrograph and Camera,YFOSC),使用棱栅Grism3分光,对超新星SN 2011fe(V波段19.5 mag)成功进行光谱观测。30 min单幅曝光,获得暗于19 mag天体的光谱,刷新了该类天体在国内观测的新的记录。该目标在光谱观测的同时有相应的测光数据以及测光标准星观测,因此星等测量误差小于0.1 mag,可以用于定量分析。 相似文献
2.
宗伟凯 付建宁 牛家树 AshleyMichaelCB 宫雪非 LawrenceJS 刘强 Luong—VanDaniel PennypackerCR StoreyJohnWV 王灵芝 王力帆 杨惠根 袁祥岩 YorkDonaldG 朱镇熹 《云南天文台台刊》2014,(1):89-94
天光背景是天文台址的一个重要指标。利用2009年位于南极冰穹A的CSTAR望远镜两个波段的观测数据,对南极冰穹A的天光背景进行了统计和分析。结果表明约74％的g波段天光背景的ADU值小于每像素100/s;90．5％的r波段的天光背景的ADU值小于每像素100／s。在不考虑大气消光的情况下,定标后的结果为2009年冰穹A的观测数据中天光背景亮度的中值：g波段为19．9mag／arcsec^2,r波段为20．1mag／aresec^2。 相似文献
3.
高精度恒星孔径测光注释 总被引：2，自引：0，他引：2
详细介绍了利用孔径测光方法得到CCD图像中恒星仪器星等的全过程,以及使用自己设计的程序对云南天文台1m望远镜观测的CCD图像进行实际测量的实验。测量结果表明:对亮星(约10mag)的内部测量精度能达到0.003mag,而对暗星(约17mag)达到0.2mag。同时,对相关问题进行深入讨论,总结了一些实验所得的经验,并与测光软件IRAF进行了内部精度的比较。 相似文献
4.
5.
SAGE(Stellar Abundance and Galactic Evolution)巡天采用一套对恒星大气参数敏感的独特测光系统,包括uSC,vSAGE,g,r,i,Hα_n,Hα_w和λ_(DDO51)(David Dunlap Observatory,DDO)共8个波段。该系统对恒星大气参数(有效温度T_(eff)、表面重力lg g和金属丰度[Fe/H])和星际消光的测量比传统的uvbyβ系统(Str?mgren-Crawford,SC)更敏感。由于g,r,i波段带宽较宽,因而观测效率较高,对恒星大气参数的测量精度和观测效率均超过uvbyβ系统和宽带测光系统。利用美国亚利桑那大学Steward天文台2.3 m Bok望远镜、新疆天文台南山1 m望远镜和乌兹别克斯坦MAO(Maidanak Astronomical Observatory)1 m望远镜已展开巡天观测。项目计划在约4年时间内完成所有的巡天观测,北天天区覆盖面积约12000(~?)~2,高精度测光(信噪比为100σ)深度约15 mag(V波段);5σ探测极限可深至约20 mag(V波段)。最终将探测约5×108颗恒星,并得出其恒星大气参数以及星际消光。该样本比之前的u,v,b,y,β测光巡天,如GCS(Geneva-Copenhagen Survey)巡天和HM(Hauck and Mermilliod 1998)巡天,扩展到更深的区域,即深度达到7～8 mag(V波段)。利用观测得到的大样本恒星测光星表,可以开展如下课题的研究:(1)得到银河系约5×10~8颗恒星大样本的金属丰度分布,并根据恒星演化模型得到其年龄分布;(2)预期搜寻到一批贫金属星候选体,并利用其他望远镜进行下一步观测;(3)结合高质量的uSC波段数据,预期可以找到一批白矮星;(4)结合其他星表,预期找到一批长周期变源以及移动天体;(5)结合uSC波段数据和其他星表,预期可以找到一批类星体。 相似文献
6.
钱伯辰 《中国科学院上海天文台年刊》1992,(13):167-169
1.56米天望远镜已于1989年上海天台的佘山工作站投入使用，经校正，瓣极轴指向偏离北极为：0″.±4″.48（在方位上）和0″.±2″.21（在高度上）。望远镜的跟踪误差也被测定：在天顶附近30分钟内所作的128次观测得到的望远镜跟踪的均方根误差为±0″.36。结果表明，1.56米望远镜的恒动跟踪十分优良。 相似文献
7.
与国家天文台兴隆站2.16m安装的北京天文台暗天体分光成像仪(BAO Faint Object Spectrograph and Camera,BFOSC)系统相似,云南天文台2.4m望远镜安装了云南暗弱天体光谱及成像仪(Yunnan Faint-Object Spectrograph and Camera,YFOSC),对它在直接照相时的CCD平场性能做了测定.使用不同旋转角度拍摄平均而得的平场,可以使不同位置拍摄的像场,所受最大误差≤0.015 mag.但与卡焦的VersArray CCD照相机不同,即使在视场中间直径6.′5的圆内,误差约在0.010～0.013 mag之间,达不到≤0.005 mag的精度. 相似文献
8.
以上海天台佘山40cm折射望远镜于1958年拍摄的3张照相底片为第一期资料,印度Kavalur的2.34m Vainu Bappu望远镜于1996年用CCD拍摄的4幅图象为第二期资料,使用Brosche等人1985年发表的球状星团NGC4147天区42颗恒星的位置和绝对自行作为参考架,用中心重叠法进行天体测量归算,得到了这个星团中心附近11'×11'天区内到B＝17.6mag为止115颗恒星的位置和绝对自行,并利用这些自行对成员概率作了估计,同时,还用Vainu Bappu望远镜的CCD进行了BVRI四色测光。本给出了这115颗恒星的位置、绝对自行和成员概率数据,同时,还给出了用Vainu Bappu望远镜的CCD获得的这些恒星的BVRI测光数据。 相似文献
9.
与国家天文台兴隆站2.16 m安装的北京天文台暗天体分光成像仪(BAO FaintObject Spectrograph and Camera,BFOSC)系统相似,云南天文台2.4 m望远镜安装了云南暗弱天体光谱及成像仪(Yunnan Faint-Object Spectrograph and Camera,YFOSC),对它在直接照相时的CCD平场性能做了测定。使用不同旋转角度拍摄平均而得的平场,可以使不同位置拍摄的像场,所受最大误差≤0.015 mag。但与卡焦的VersArray CCD照相机不同,即使在视场中间直径6.’5的圆内,误差约在0.010～0.013 mag之间,达不到≤0.005 mag的精度。 相似文献
10.
上海台1．56m望远镜新CCD照相机系统 总被引：3，自引：0，他引：3
介绍了安装在中国科学院上海天台1．56m望远镜上的新CCD照相机系统，内容涉及CCD的量子效率、增益、控制器、观测程序以及滤光片等情况，为使用该1．56m望远镜的天学家提供了所需的参数。 相似文献
11.
Photoelectric observations of night sky brightness at different zenith distances in blue, yellow and red colours have been
carried out at Abu-Simbel site. Variations in the night sky brightness and (B-V) colour index with time are detected. These
variations have been explained by the change of the galactic latitude of the observed point with time. The deduced results
of night sky brightness have been compared with that obtained before at other sites. It has been found for both blue and yellow
colours, that Abu-Simbel is the darkest site especially for zenith distances equal or greater than 60°. The present values
of night sky brightness and colour have been obtained for the first time at Abu-Simbel site. The average night sky brightness
at the galactic plane is 22.58 mag/arc sec2 for blue and 21.66 mag/arc sec2 for yellow.
This revised version was published online in August 2006 with corrections to the Cover Date. 相似文献
12.
Photoelectric measurements of the night sky brightness and the light pollution of Kottamia Observatory have been carried out and the deduced results are expressed in mag/sec2. The maximum brightness of the sky in the direction of Cairo city at zenith distance 45° and azimuth 70° when the sun is almost 60° below the horizon are 22.68; 21.54 and 19.82 mag/sec2 for blue, yellow and red colours respectively. The corresponding values of night sky background are 22.94; 21.85 and 20.14 mag/sec2 respectively.The isophotes of the sky brightness at Kottamia Observatory have been drawn for blue, yellow and red colours. The variations of the night sky brightness and the (B-V) colour index with altitude of the observed point have been studied.The light pollution and the night sky brightness at the site of Kottamia Observatory is compared with that deduced by different investigators at other sites. It has been shown that the sky brightness at zenith distance 45° at Kottamia Observatory site is similar to Kitt Peak and Palomar Observatory sites. Kottamia Observatory site is slightly brighter than Junipero Serra while it is darker than Mount Hamilton and San Jose sites. The comparative results have been carried out at blue and yellow colours. No comparison is obtained at red as there is no data published for the red colour. 相似文献
13.
S. Nawar 《Astrophysics and Space Science》1998,262(4):477-483
Photoelectric measurements have been carried out at Kottamia Observatory site to study night sky brightness and the atmospheric
extinction at different wavelengths. The results show that the mean extinction coefficients are k = 0.41, k = 0.28< and k
= 0.17 mag/air mass during autumn season. These values are almost the same as that obtained by Mikhail (1979) at the same
site during the same season. Results of night sky brightness at different altitudes above the horizon have been obtained.
Complete scan each five degrees step in azimuth have been done at altitudes 50°, 60° and 70° to complete the previous measurements
given by Nawar et al. (1995). Far from the diffuse galactic light, slight variations in night sky brightness with azimuth
have been detected.
This revised version was published online in August 2006 with corrections to the Cover Date. 相似文献
14.
We report measurements from which we determine the spatial structure of the lunar contribution to night sky brightness, taken at the LSST site on Cerro Pachon in Chile. We use an array of six photodiodes with filters that approximate the Large Synoptic Survey Telescope’s u, g, r, i, z, and y bands. We use the sun as a proxy for the moon, and measure sky brightness as a function of zenith angle of the point on sky, zenith angle of the sun, and angular distance between the sun and the point on sky. We make a correction for the difference between the illumination spectrum of the sun and the moon. Since scattered sunlight totally dominates the daytime sky brightness, this technique allows us to cleanly determine the contribution to the (cloudless) night sky from backscattered moonlight, without contamination from other sources of night sky brightness. We estimate our uncertainty in the relative lunar night sky brightness vs. zenith and lunar angle to be between 0.3–0.7 mags depending on the passband. This information is useful in planning the optimal execution of the LSST survey, and perhaps for other astronomical observations as well. Although our primary objective is to map out the angular structure and spectrum of the scattered light from the atmosphere and particulates, we also make an estimate of the expected number of scattered lunar photons per pixel per second in LSST, and find values that are in overall agreement with previous estimates. 相似文献
15.
An interferometric astrometric mission, aiming at accuracies at around the10 microarcsec level, was recommended as a high priority concept within thenew ESA Horizon 2000+ scientific programme. The original outline concept forsuch a mission, GAIA, presented its general feasibility but did not addressmany questions of implementation or optimisation. Another concept of aninterferometer for a scanning astrometric satellite is presented. It containsa simpler optical telescope and a more efficient detector system. The designutilizes the full resolution of all light in the dispersed fringes of aFizeau interferometer. A preliminary optimization of the satellite indicatesthat two telescope units with a baseline of 100 cm will achieve a precisionof 3, 8, 22, 68, 302 microarcsec for parallaxes of stars with V = 12, 14, 16, 18, 20 mag, respectively, from a 5 year mission. Simultaneousspectrophotometry of the entire spectrum of each star will be obtained with aresolution corresponding to intermediate band photometry. The expectedprecision of this photometry is about 0.003 mag for V = 16. The performance is good in crowded fields, at least up to one star per 5 arcsec2. A Hipparcos-type beam combiner of 150 cm width is placed in front of atelescope with 4 square apertures of 50 cm. The assumed focal length is f = 60 m and the field 0.5 degree diameter. The detector consists of CCDs used for time delayed integration (drift-scan.) 相似文献
16.
The first World Atlas of the artificial night sky brightness 总被引：5，自引：0，他引：5
P. Cinzano F. Falchi C.D. Elvidge 《Monthly notices of the Royal Astronomical Society》2001,328(3):689-707
We present the first World Atlas of the zenith artificial night sky brightness at sea level. Based on radiance-calibrated high-resolution DMSP satellite data and on accurate modelling of light propagation in the atmosphere, it provides a nearly global picture of how mankind is proceeding to envelop itself in a luminous fog. Comparing the Atlas with the United States Department of Energy (DOE) population density data base, we determined the fraction of population who are living under a sky of given brightness. About two-thirds of the World population and 99 per cent of the population in the United States (excluding Alaska and Hawaii) and European Union live in areas where the night sky is above the threshold set for polluted status. Assuming average eye functionality, about one-fifth of the World population, more than two-thirds of the United States population and more than one half of the European Union population have already lost naked eye visibility of the Milky Way. Finally, about one-tenth of the World population, more than 40 per cent of the United States population and one sixth of the European Union population no longer view the heavens with the eye adapted to night vision, because of the sky brightness. 相似文献
17.
Naosuke Sekiguchi 《Earth, Moon, and Planets》1971,2(4):423-434
An anomalous enhancement of brightness of the lunar surface was observed on March 26, 1970, during photometric and polarimetric observations of the Moon made by the 91-cm reflector of the Dodaira Station of the Tokyo Astronomical Observatory. The region near the Aristarchus was 0.3 mag. brighter compared with that corresponding to the ordinary brightness variation curve. The polarimetric results also showed evidence quite consistent with the phenomenon of the luminescence. The colour index diminished by about 0.1 mag. The results of the photographic photometry also confirmed the enhancement of brightness over a wide part of the lunar surface that night. This brightening may be related to the large solar flare observed on March 25, 12h UT, 1970, twenty-nine hours before our observations. 相似文献
18.
S. J. Collander-Brown A. Fitzsimmons E. Fletcher M. J. Irwin I. P. Williams 《Monthly notices of the Royal Astronomical Society》1999,308(2):588-592
We have obtained a number of CCD images of two trans-Neptunian objects, 1994 VK8 and 1996 TP66, over two nights. The changes in magnitude of these objects have been examined, in a search for periodic variation. In the case of 1996 TP66, nothing other than random noise can be found to within the errors of ∼0.04 mag. Although a periodic signal is found for 1994 VK8, it appears to be an artefact, as the same frequency appears in the variation of sky brightness and is probably due to the sampling of the data. However, 1994 VK8 does exhibit a variation of ∼0.5 mag. This would suggest either significant non-sphericity or a change in surface composition over a large area. In either case 1994 VK8 warrants further investigation. 相似文献
19.
E. Massaro R. Nesci M. Maesano F. Montagni & F. D'Alessio 《Monthly notices of the Royal Astronomical Society》1998,299(1):47-50
We present the results of photometric observations of BL Lacertae at 1 μm performed during the strong outburst that occurred in the summer of 1997. Measurements were carried out using the F99 filter of the Arizona system. Simultaneous observations in the B V bands were made with other telescopes. Large and fast variations were observed on the night of August 2 when the brightness of BL Lacertae changed by ∼ 0.5 mag in about 2 h: the variation amplitude is greater at higher frequency. Some implications of these results for the origin of the fast variations are discussed. We also report the first F99 calibration for three reference stars in the BL Lac field. 相似文献
20.
C. &#;banolu S. Evren G. Ta&#; Ö. Çak&#;rl&#; 《Monthly notices of the Royal Astronomical Society》2005,360(3):1077-1084
The post-common envelope and pre-cataclysmic binary V471 Tau has been observed by the authors since 1973. At least a complete light curve in B and V bands and more than two eclipse timings were obtained in each year. All the available data published so far (including the authors') have been collected and analysed for the brightness and orbital period changes. The system brightened about 0.22 mag in both B and V bands more or less regularly up to 1997 and started to decrease afterwards. A search for periodicity of this variation yields a period longer than 85 yr. In addition to this long-period variation, a small amplitude of about 0.08 mag and short time-interval fluctuations on the mean brightness have been detected. The variations of the mean brightness have been discussed and plausible causes suggested. The changes of the apparent period have been attributed to a third body. Analysis of all the 'observed−calculated' (O−C) data yields a period of 32.4 yr, with a semi-amplitude of 151 s and an eccentricity of 0.30 for the third-body orbit. For orbital inclinations greater than 34° the mass of the third body would possibly match to a brown dwarf. One of the most interesting features in the light curve of V471 Tau is the decrement of the eclipse depth with time. The depth of the eclipse in the B band has been decreased from 0.082 to 0.057 mag over 34 yr. Subtracting the variation of the depth due to the brightening of the red dwarf star, the actual variation in depth, originated from from the white dwarf, was found to be about 0.012 mag. This change in the brightness of the compact object has been attributed to the mass accretion from its primary component via thermally driven wind and/or flare-like events. 相似文献