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1.
2021年6月,使用南京大学本科实验教学的65 cm反射式望远镜系统,对其后端的电荷耦合器件(Charge-Coupled Device, CCD)的性能采用圆顶平场法进行了实际测定,得到了CCD相机的快门函数;同时用平场序列曝光,检测了CCD相机的线性。CCD相机的读出值从0到61 900模数转换单位(Analog-Digital Unit, ADU)非线性小于1%,同时CCD相机的増益为1.02e-/adu,读出噪音为13e-。但对于恒星这样的点光源的观测,当像元的数值高于38 000 adu时产生溢出。因此,在使用本CCD相机做点光源观测研究时,需要选择恰当的曝光时间,避免星像溢出。实际天文观测中,利用此研究得到的快门函数可以对观测图像进行校准,有效提高测光精度。 相似文献
2.
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 相似文献
3.
姚保安 《中国科学院上海天文台年刊》2004,(1)
1 .5 6m望远镜新CCD系统是在里克天文台用其控制电路组装而成的。该系统能在MPP模式与非MPP模式之间自由快速转换。我们比较了两种模式的性能差异 ,得到 :(1)增益和读出噪音不变。 (2 )在 - 10 0℃温度 ,MPP模式的暗流对短的或中等长度的露光可以忽略 ,并且暗流对CCD芯片的温度变化不太敏感 ;非MPP模式的暗流有确定的图案 ,对CCD的温度变化比MPP敏感。因此稳定的低温是必须的 ,并且使用时须减暗流。 (3)使用MPP的代价是 ,相对于非MPP模式 ,动态范围至少减小约 90 0 0adu(增益 4 .6e- /adu)。用户使用时应按照科学目的选择模式。 相似文献
4.
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。 相似文献
5.
GPS掩星折射率剖面一维变分同化 总被引：11，自引：1，他引：10
近年来,GPS／LEO(全球定位系统／低地球轨道)卫星无线电掩星技术给出了地球大气探测的新途径．从LEO卫星观测到的掩星数据可以反演的地球大气的气压、水汽、温度等剖面;它们对气象和大气科学研究,是具有潜在价值的数据资源．掩星数据资料的同化技术可以有效地改进这些气象参数的剖面,从而改进目前的数值天气预报模式．在当前采用的一维变分同化反演技术中,可以用掩星观测资料的大气折射率或弯曲角剖面进行同化,来反演大气水汽和温度剖面以及海平面压强．作为独立自主开发的GPD／LEO掩星技术系统的一部分,以欧洲中尺度天气预报分析(ECMWF)资料为背景场,CHAMP 掩星观测得到的折射率剖面为观测值,采用Levenberg—Marquardt方法实行GPS掩星资料一维变分同化．在讨论中,用掩星观测点附近相应的探空气球资料来检验CHAMP掩星资料变分同化的结果． 相似文献
6.
大气视宁度严重影响了地面望远镜观测的成像分辨率。对于直径ｒＬ的单孔镜，Ｆｒｉｅｄ给出恒星光波波前到达角的均方差为＜α２＞＝０．３５８（λｒＬ）１／３（λｒ０）５／３这一公式被很多文献所采用，并推广应用于双瞳视宁度仪测量，等等。事实上，Ｙｕｒａ和Ｔａｖｉｓ（１９８５）指出，恒星光波波前的瞬间倾角与星像重心在焦平面的角位置并不完全相关，波前倾角的方差与焦平面重心的方差也是不一致的。实际测量中，我们常使用的是焦平面像重心的测量。因此，使用的公式应当有所修正。本文从Ｔａｔａｒｓｋｉ的理论公式出发，更简捷地得到了同样的结果。即，所使用的公式应修改为＜α２＞＝０．３３９（λｒＬ）１／３（λｒ０）５／３与此有关的视宁度测量公式中的其他常数也需修改 相似文献
7.
大气角动量资料源的变化对研究日长变化激发的贡献 总被引：4，自引：0，他引：4
本文采用1979—1995年间由空间大地测量技术观测和归算的日长变化（△LOD）序列,以及由美国国家气象中心（NMC）和美国国家环境预测中心与美国国家大气研究中心（NCEP／NCAR）利用全球气象资料各自归算的大气角动量（AAM）序列,重新分析、研究和估计了大气对△LOD的激发作用,比较了上述各个大气角动量序列对△LOD激发贡献,得到的主要结果如下：1．NCEP／NCAR用同化后的全球气象资料重新归算的AAM序列比原来NMC的序列具有系统均匀化、噪声小和分辨率高的特点,以及和日长变化的符合度更好．2．采用NCEP／NCAR重新归算的AAM来研究大气在从亚季节性到年际时间尺度上对非潮汐△LOD的激发贡献,得到进一步改善的结果,尤其是在准两年时间尺度上．但是大气仍不能解释全部△LOD化,可能存在其它激发源．3．大气对△LOD高频潮汐项的估计值影响较小,并从△LOD中解算出周年和半年潮汐参数估计的初步结果． 相似文献
8.
大气折射是天体测量最基本的问题之一，它影响着天体位置测定的精度。气象资料自动采集系统是自动计算大气折射必不可少的仪器，为观测结果和气象的相关分析提供了可能．本文介绍的气象资料自动采集系统，可实时采集并可用于其它天文观测仪器． 相似文献
9.
介绍了Be星的基本特性．评述了近年来对Be星星周物质结构研究的成果．重点介绍了最新的关于Be星星周盘产生和变化的动力学模型．另外，对Be／X射线双星系统的研究也做了简要评述，重点论述了致密星与Be星延伸大气的相互作用． 相似文献
10.
使用移动式亚毫米波望远镜(POST)在位于青藏高原海拔3200米的紫金山天文台德令哈射电天文观测站址测量地球大气492GHz频率处天顶方向的不透明度(τ0)的结果．在1999—2000年冬季和2000—2001年冬季的两个观测季节内累计共进行了约870个小时的测量，取得了25842组τ0的有效数据．对数据的统计表明，观测季节内τ0值主要分布在1．5—3．0之间．观测时段内大气不透明度τ0≤1．0的时间比例约占3％．在给出实测资料的基础上，将所测量的亚毫米波不透明度与国际现有亚毫米波台址的不透明度进行了初步比较． 相似文献
11.
Laura Schaefer 《Icarus》2004,169(1):216-241
We modified the MAGMA chemical equilibrium code developed by Fegley and Cameron (1987, Earth Planet. Sci. Lett. 82, 207-222) and used it to model vaporization of high temperature silicate lavas on Io. The MAGMA code computes chemical equilibria in a melt, between melt and its equilibrium vapor, and in the gas phase. The good agreement of MAGMA code results with experimental data and with other computer codes is demonstrated. The temperature-dependent pressure and composition of vapor in equilibrium with lava is calculated from 1700 to 2400 K for 109 different silicate lavas in the ONaKFeSiMgCaAlTi system. Results for five lavas (tholeiitic basalt, alkali basalt, Barberton komatiite, dunite, and a molten type B1 Ca, Al-rich inclusion) are discussed in detail. The effects of continuous fractional vaporization on chemistry of these lavas and their equilibrium vapor are presented. The predicted abundances (relative to Na) of K, Fe, Si, Al, Ca, and Ti in the vapor equilibrated with lavas at 1900 K are lower than published upper limits for Io's atmosphere (which do not include Mg). We predict evaporative loss of alkalis, Fe, and Si during volcanic eruptions. Sodium is more volatile than K, and the Na/K ratio in the gas is decreased by fractional vaporization. This process can match Io's atmospheric Na/K ratio of 10±3 reported by Brown (2001, Icarus 151, 190-195). Silicon monoxide is an abundant species in the vapor above lavas. Spectroscopic searches are recommended for SiO at IR and mm wavelengths. Reactions of metallic vapors with S- and Cl-bearing volcanic gases may form other unusual gases including MgCl2, MgS, MgCl, FeCl2, FeS, FeCl, and SiS. 相似文献
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13.
《中国天文和天体物理学报》2014,(10)
正Research in Astronomy and Astrophysics publishes original research papers and reviews on all branches of astronomy and astrophysics.Reviews are by invitation only.Important new results that require rapid publication can be submitted as a Letter(Letters must be restricted in length to 6 printed pages).Authors who submit a paper are expected to be able to certify that the paper is original work, 相似文献
14.
15.
Laura Schaefer 《Icarus》2005,173(2):454-468
We use chemical equilibrium calculations to model the speciation of alkalis and halogens in volcanic gases emitted on Io. The calculations cover wide temperature (500-2000 K) and pressure (10−6 to 10+1 bars) ranges, which overlap the nominal conditions at Pele (T=1760 K, P=0.01 bars). About 230 compounds of 11 elements (O, S, Li, Na, K, Rb, Cs, F, Cl, Br, I) are considered. The elemental abundances for O, S, Na, K, and Cl are based upon observations. CI chondritic elemental abundances relative to sulfur are used for the other alkalis and halogens (as yet unobserved on Io). We predict the major alkali species in Pele-like volcanic gases and the percentage distribution of each alkali are LiCl (73%), LiF (27%); NaCl (81%), Na (16%), NaF (3%); KCl (91%), K (5%), KF (4%); RbCl (93%), Rb (4%), RbF (3%); CsCl (92%), CsF (6%), Cs (2%). Likewise the major halogen species and the percentage distribution of each halogen are NaF (88%), KF (10%), LiF (2%); NaCl (89%), KCl (11%); NaBr (89%), KBr (10%), Br (1%); NaI (61%), I (30%), KI (9%). We predict the major halogen condensates and their condensation temperatures at P=0.01 bar are NaF (1115 K), LiF (970 K); NaCl (1050 K), KCl (950 K); KBr (750 K), RbBr (730 K), CsBr (645 K); and solid I2 (200 K). We also model disequilibrium chemistry of the alkalis and halogens in the volcanic plume. Based on this work and our prior modeling for Na, K, and Cl in a volcanic plume, we predict the major loss processes for the alkali halide gases are photolysis and/or condensation onto grains. Their estimated photochemical lifetimes range from a few minutes for alkali iodides to a few hours for alkali fluorides. Condensation is apparently the only loss process for elemental iodine. On the basis of elemental abundances and photochemical lifetimes, we recommend searching for gaseous KCl, NaF, LiF, LiCl, RbF, RbCl, CsF, and CsCl around volcanic vents during eruptions. Based on abundance considerations and observations of brown dwarfs we also recommend a search of Io's extended atmosphere and the Io plasma torus for neutral and ionized Li, Cs, Rb, and F. 相似文献
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17.
Li Xin-nan Zhang Hai-ying Cui Xiang-qun Jiang Zi-bo Zheng Yi Liu Xing-tao Ni Hou-kun 《Chinese Astronomy and Astrophysics》2012
A special stressed annular polishing technique is proposed to mill the off-axis aspheric sub-mirrors of a large segmented mirror with an annular polishing machine. Based on the basic principle of stressed annular polishing technique, a set of special stressing mechanisms are designed to convert milling the aspheric surfaces of sub-mirrors with different off-axis distances into milling the spherical surfaces with identical radii of curvature, so that they can be pol- ished simultaneously on a continuous polishing machine. It took about contin- uous 40 hours to polish a scaled-down mirror of the planning Chinese Future Giant Telescope (CFGT) using this technique. This mirror has the 330 mm di- ameter, 3.6 m off-axis distance, and the 21.6 m radius of curvature, and its max- imum asphericity is 16 micron. The experiment shows that this method has a high effciency, suits batch manufacturing, especially the batch manufacturing of aspheric sub-mirrors of the segmented primary mirror of an extremely large aperture telescope. 相似文献
18.
In this paper, we investigate the dynamics of Born–Infeld (B–I) phantom model in the ω–ω′ plane, which is defined by the equation of state parameter for the dark energy and its derivative with respect to N (the logarithm of the scale factor a). We find the scalar field equation of motion in ω–ω′ plane, and show mathematically the property of attractor solutions which correspond to ω
φ
∼−1, Ω
φ
=1, which avoid the “Big rip” problem and meets the current observations well.
相似文献
19.
In astronomical observations at optical wavelengths, a fast image tracking system can be adopted to reduce the effects of the atmospheric seeing and telescopic tracking error, and therefore improve the observing efficiency. Aiming at the need of astronomical observations, totally 5 kinds of algorithms in two categories were selected to make a comparative study on their accuracies and stabilities under different noise conditions by both numerical experiment and laboratory test. The results indicate that the normalized cross-correlation method and barycenter method have not only a higher accuracy but also a better reliability against interferences, they will be applied to the high-resolution spectrograph of the Xinglong 2.16 m telescope and the scienti?c instruments of the SONG (Stellar Observations Network Group) project, respectively. 相似文献
20.
Marcelo Samuel Berman 《Astrophysics and Space Science》2008,314(1-3):79-82
A combined BCDE (Brans-Dicke and Einstein-Cartan) theory with lambda-term is developed through Raychaudhuri’s equation, for
inflationary scenario. It involves a variable cosmological constant, which decreases with time, jointly with energy density,
cosmic pressure, shear, vorticity, and Hubble’s parameter, while the scale factor, total spin and scalar field increase exponentially.
The post-inflationary fluid resembles a perfect one, though total spin grows, but the angular speed does not (Astrophys. Space
Sci. 312: 275, 2007d).
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