共查询到19条相似文献，搜索用时 171 毫秒
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现有标准设计的反光望远镜在拍摄CCD平场时,绝大多数都受残留散射光的影响.但是赤道式与地平式反光镜所受影响是不同的.在赤道式上做时间序列较差测光时,只要待测星永远位于CCD的固定像元上,不太准确的CCD平场也能得到高精度的测光结果.当需要0.1%～0.3%精度的平场时,则可以采用夜天平场.地平式的特点是,它的CCD相机必须置于旋转器上,在跟踪天体时不停地旋转,以抵消地球自转的影响.上述用于赤道式的方法失效,因此,在CCD平场时,消除散射光的影响比赤道式更为重要.一个典型的地平式反光镜的例子是NAOC兴隆天文台的EOS 1米镜.虽然该台已附加了防散射光的装置,但是对所有B、V、R、I滤光片,在不同旋转器位置拍摄的CCD平场,仍然有2%～3%的差别(主要是梯度).该文给出了改进的建议,必须满足下面两个条件:Cij=C(r);旋转器的中心与反光镜的光学中心重合.此问题的解决对所有地平式反光望远镜都有普遍意义. 相似文献
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关于CCD平场快门效应的改正及有关问题 总被引：4，自引：0，他引：4
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． 相似文献
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一个巨型望远镜方案 总被引：4，自引：0，他引：4
提出一个有特色的巨型望远镜(FGT)方案．其主镜口径为30米，主焦比为1．2，由1095块圆环形子镜构成．采用地平式装置．光学系统包括Nasmyth系统、折轴(Coude)系统和一个大视场系统．提出一个由4个镜面组成的新的Nasmyth系统，在约10′的视场范围内像斑小于爱里斑，达到衍射极限．比传统的Nasmyth系统的衍射极限视场大得多．可在这样的大视场内同时作好几个小区域的衍射极限的观测．当由Nasmyth系统转换到折轴系统和大视场系统时，采用主动光学技术改变子镜的面形、倾斜和平移，产生一个新的主镜面形，使折轴系统和大视场系统都能得到很好的像质．大视场系统的视场直径25′，场曲轻微，并有可能校正大气色散．给出了子镜面形和位置的公差，并讨论了望远镜的装置和结构,方案中的特色和创新对未来大望远镜的研制有普遍意义． 相似文献
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安装于云南天文台 1米反光镜上的新Tek 1 0 2 4× 1 0 2 4CCD相机是很好的系统 ,它的某些性能已在文 [1 ],[2 ],[3]中报导。自 1 998年 7月起此相机的有关机械部分已重做 ,并且CCD芯片也被另一片类似的Tek 1 0 2 4× 1 0 2 4代替。但原来的滤光片末换 ,不幸 ,这些玻璃滤光片都已霉变。霉菌侵入玻璃内部 ,使滤光片难以复原 ,企图用平场来改正这种影响不能成功。在这段时期内 ,所有使用了这些滤光片的测光都有可能受影响。当更换了B滤光片后 ,B星等已正常。其它滤光片也在准备更换中。 相似文献
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一架望远镜的质量不仅取决于其光学零件的质量，同时不取于整个机械结构的优劣。因此，机械设计在望远镜制造中占有极其翻天覆地的地位，对于一架现有望远镜的改装，机械设计的难度更大。本文介绍用于改 装双筒望远镜的φ85厘米反射望远镜镜筒的设计和结构分析。由于EM－1赤道的承载能力有限，镜筒设计中如何重量成为设计的关键问题。为此，镜筒的主要部位，诸如筒体和主镜室等均作过力学分析，选择其中最佳的方案。该镜筒将作为一个完整的镜筒安装在EM－1装置上，它主要用于光电测光工作，也可以作光谱工作。 相似文献
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海尔—波普彗星喷流的一次成功检测 总被引：2，自引：0，他引：2
上海天文台余山观测站1．56m望远镜于1996年9月23日北京时间19点40分拍摄了海尔-波普彗星的CCD图象。使用的滤光片是R，露光时间为45s。经过偏流（bias）、暗流（dark）以及平场（flat）改正的图象上可以看出彗核附近有5条喷流，但是并不十分清楚（见图1）。这主要是由于喷流叠 相似文献
7.
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
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莱曼阿尔法太阳望远镜(LST)是先进天基太阳天文台(ASO-S)卫星的载荷之一,它包括白光太阳望远镜(WST),全日面太阳成像仪(SDI)和日冕仪(SCI)等仪器. 1991年Kuhn, Lin和Loranz提出的方法(简称KLL方法)是WST和SDI在轨平场定标的方法之一.为了研究WST和SDI的平场定标精度对KLL方法的相邻位置时间间隔的敏感性,使用太阳动力学观测卫星(SDO)的日震和磁成像仪(HMI)及太阳大气成像仪(AIA)的全日面成像观测数据测试和分析在使用KLL方法时相邻位置时间间隔对所得平场精度的影响.结果显示在LST使用KLL方法进行平场定标时,相邻位置时间间隔越短越好.具体分析表明,WST平场精度对相邻位置采样时间间隔不敏感,而SDI时间间隔需要在240 s范围内.分析结果对卫星姿态调整到稳定所需的时间给出了一定限制. 相似文献
11.
T. Guillot L. Abe A. Agabi J.‐P. Rivet J.‐B. Daban D. Mkarnia E. Aristidi F.‐X. Schmider N. Crouzet I. Gonalves C. Gouvret S. Ottogalli H. Faradji P.‐E. Blanc E. Bondoux F. Valbousquet 《Astronomische Nachrichten》2015,336(7):638-656
The installation and operation of a telescope in Antarctica represent particular challenges, in particular the requirement to operate at extremely cold temperatures, to cope with rapid temperature fluctuations and to prevent frosting. Heating of electronic subsystems is a necessity, but solutions must be found to avoid the turbulence induced by temperature fluctuations on the optical paths. ASTEP 400 is a 40cm Newton telescope installed at the Concordia station, Dome C since 2010 for photometric observations of fields of stars and their exoplanets. While the telescope is designed to spread star light on several pixels to maximize photometric stability, we show that it is nonetheless sensitive to the extreme variations of the seeing at the ground level (between about 0′′.1 and 5′′) and to temperature fluctuations between –30°C and –80 °C. We analyze both day‐time and night‐time observations and obtain the magnitude of the seeing caused by the mirrors, dome and camera. The most important effect arises from the heating of the primary mirror which gives rise to a mirror seeing of 0′′.23 K–1. We propose solutions to mitigate these effects. (© 2015 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim) 相似文献
12.
T. M. Gledhill A. N. Witt U. P. Vijh C. J. Davis 《Monthly notices of the Royal Astronomical Society》2009,392(3):1217-1224
Imaging polarimetry through J and H broad-band filters and a 3.4 μm narrow-band filter is used to highlight the regions of scattered light in the Red Rectangle. We find that the scattered light identifies the circumbinary dust component of the molecular disc seen in CO emission. This region also appears to be the origin of the recently discovered Blue Luminescence. We find that the degrees of polarization are consistent with the amorphous carbon dust model invoked by Men'shchikov. Spectropolarimetry from 1.4 to 2.5 μm confirms that the degree of polarization in the central arcsecond region is very low. This suggests that the central bicone seen in the near-infrared is predominantly due to emission from hot dust and/or from stochastically heated nanoparticles, rather than due to scattering by large grains. 相似文献
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Roelof S. de Jong 《Monthly notices of the Royal Astronomical Society》2008,388(4):1521-1527
Measuring the integrated stellar halo light around galaxies is very challenging. The surface brightness of these haloes is expected to be many magnitudes below dark sky and the central brightness of the galaxy. Here, I show that in some of the recent literature the effect of very extended Point Spread Function (PSF) tails on the measurements of halo light has been underestimated; especially in the case of edge-on disc galaxies. The detection of a halo along the minor axis of an edge-on galaxy in the Hubble Ultra Deep Field can largely be explained by scattered galaxy light. Similarly, depending on filter and the shape one assumes for the uncertain extended PSF, 20–80 per cent of the halo light found along the minor axis of scaled and stacked Sloan Digital Sky Survey (SDSS) edge-on galaxy images can be explained by scattered galaxy light. Scattered light also significantly contributes to the anomalous halo colours of stacked SDSS images. The scattered light fraction decreases when looking in the quadrants away from the minor axis. The remaining excess light is well modelled with a Sérsic profile halo with shape parameters based on star count halo detections of nearby galaxies. Even though, the contribution from PSF scattered light does not fully remove the need for extended components around these edge-on galaxies, it will be very challenging to make accurate halo light shape and colour measurements from integrated light without very careful PSF measurements and scattered light modelling. 相似文献
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为检测微弱的射电信号,要求望远镜接收机噪声性能良好.低噪声放大器(Low Noise Amplifier, LNA)作为接收机前端关键电路,其噪声系数和增益决定了整机的噪声性能.设计了一款1.2–2.2 GHz的低噪声放大器,电路采用两级级联结构,第2级通过引入负反馈,在改善增益平坦度和拓宽带宽的同时减小噪声,级间经过后级输入阻抗优化后仅需一个隔直电容.并引入有损输出匹配网络,实现高增益、低噪声、良好回波损耗和较为平坦的宽带LNA设计.测试结果表明,在1.2–2.2 GHz频段增益30–33 dB,噪声温度平均值为47 K,输出1 d B压缩点大于11.3 dBm.测试性能良好,可用于该频段接收机系统中. 相似文献
15.
We check the performance of the FRODOSpec integral‐field spectrograph for observations of faint sources in crowded fields. Although the standard processing pipeline L2 yields too noisy fibre spectra, we present a new processing software (L2LENS) that gives rise to accurate spectra for the two images of the gravitationally lensed quasar Q0957+561. Among other things, this L2LENS reduction tool accounts for the presence of cosmic‐ray events, scattered‐light backgrounds, blended sources, and chromatic source displacements due to differential atmospheric refraction. Our non‐standard reduction of Q0957+561 data shows the ability of FRODOSpec to provide useful information on a wide variety of targets, and thus, the big potential of integral‐field spectrographs on current and future robotic telescopes. (© 2014 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim) 相似文献
16.
In this paper we present an interference detection toolbox consisting of a high dynamic range Digital Fast‐Fourier‐Transform spectrometer (DFFT, based on FPGA‐technology) and data analysis software for automated radio frequency interference (RFI) detection. The DFFT spectrometer allows high speed data storage of spectra on time scales of less than a second. The high dynamic range of the device assures constant calibration even during extremely powerful RFI events. The software uses an algorithm which performs a two‐dimensional baseline fit in the time‐frequency domain, searching automatically for RFI signals superposed on the spectral data. We demonstrate, that the software operates successfully on computer‐generated RFI data as well as on real DFFT data recorded at the Effelsberg 100‐m telescope. At 21‐cm wavelength RFI signals can be identified down to the 4σ rms level. A statistical analysis of all RFI events detected in our observational data revealed that: (1) mean signal strength is comparable to the astronomical line emission of the Milky Way, (2) interferences are polarised, (3) electronic devices in the neighbourhood of the telescope contribute significantly to the RFI radiation. We also show that the radiometer equation is no longer fulfilled in presence of RFI signals. (© 2007 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim) 相似文献
17.
云南1m太阳塔真空封窗减反射膜的设计 总被引：1，自引：0，他引：1
云南1m太阳塔(YNST)[1]是一个真空结构的塔式太阳望远镜,依靠4块平板封窗玻璃把整个光学系统密封在真空系统中。封窗玻璃的引入,不仅会对太阳光有一定的吸收和反射,使来自太阳辐射的能量有一定的损失,并会形成杂散光,影响成像质量。本文讨论了这些影响。根据云南1m红外太阳塔科学指导委员会确定的工作波段的要求,设计了一种膜系设计方法,可以利用最少的膜系层数来达到需要的结果。并用一组材料进行了模拟设计实验,获得了较为理想的优化结果,在关键波长处显著减小了反射率,减少了杂散光的形成。这种设计方法很适合象太阳塔这种很宽的波段里面对一组波长有很高要求的设计任务,将大大提高光能利用率,具有重要的价值。 相似文献
18.
D. Heath Jones Patrick L. Shopbell Joss Bland-Hawthorn 《Monthly notices of the Royal Astronomical Society》2002,329(4):759-774
The past 5 years have seen a rapid rise in the use of tunable filters in many diverse fields of astronomy, through Taurus Tunable Filter (TTF) instruments at the Anglo-Australian and William Herschel Telescopes. Over this time we have continually refined aspects of operation and developed a collection of special techniques to handle the data produced by these novel imaging instruments. In this paper, we review calibration procedures and summarize the theoretical basis for Fabry–Perot photometry that is central to effective tunable imaging. Specific mention is made of object detection and classification from deep narrow-band surveys containing several hundred objects per field. We also discuss methods for recognizing and dealing with artefacts (scattered light, atmospheric effects, etc.), which can seriously compromise the photometric integrity of the data if left untreated. Attention is paid to the different families of ghost reflections encountered, and the strategies used to minimize their presence. In our closing remarks, future directions for tunable imaging are outlined and contrasted with the Fabry–Perot technology employed in the current generation of tunable imagers. 相似文献
19.
J. Larsson G. Miniutti A. C. Fabian J. M. Miller C. S. Reynolds G. Ponti 《Monthly notices of the Royal Astronomical Society》2008,384(4):1316-1326
We report on a 151-ks net exposure Suzaku observation of the narrow-line Seyfert 1 galaxy Mrk 335. The 0.5–40 keV spectrum contains a broad Fe line, a strong soft excess below about 2 keV and a Compton hump around 20–30 keV. We find that a model consisting of a power law and two reflectors provides the best fit to the time-averaged spectrum. In this model, an ionized, heavily blurred, inner reflector produces most of the soft excess, while an almost neutral outer reflector (outside ∼ 40 r g ) produces most of the Fe line emission. The spectral variability of the observation is characterized by spectral hardening at very low count rates. In terms of our power-law + two-reflector model it seems like this hardening is mainly caused by pivoting of the power law. The rms spectrum of the entire observation has the curved shape commonly observed in active galactic nuclei, although the shape is significantly flatter when an interval which does not contain any deep dip in the light curve is considered. We also examine a previous 133-ks XMM–Newton observation of Mrk 335. We find that the XMM–Newton spectrum can be fitted with a similar two-reflector model as the Suzaku data and we confirm that the rms spectrum of the observation is flat. The flat rms spectra, as well as the high-energy data from the Suzaku PIN detector, disfavour an absorption origin for the soft excess in Mrk 335. 相似文献