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1.
硅微条探测器空间分辨率高、工作性能稳定, 广泛地应用于空间高能粒子探测领域. 如费米gamma射线空间望远镜(Fermi Gamma-ray Space Telescope, FGST)以及阿尔法磁谱仪(Alpha Magnetic Spectrometer 2, AMS-02)的径迹探测器中都采用了高位置分辨率的硅微条探测器. 基于硅微条探测器在空间观测领域的应用前景, 针对硅微条探测器单元设计了一套低噪声的电子学读出系统. 整个电子学系统分为前端电子学、数据获取电路和上位机软件. 前端电子学为提高集成度, 采用了一款电荷读出芯片VATAGP8, 实现了多通道、低噪声的电荷信号测量; 数据获取电路使用现场可编程门阵列(Field Programmable Gate Array, FPGA)实现了对前端电子学的时序控制以及对测量信号的采集控制; 上位机用来接收、处理数据获取电路采集的信号数据. 在对电子学通道的线性、基线、噪声等性能进行测试之后, 得到系统在0--200fC电荷输入范围内的线性增益约为13.41bin/fC, 积分非线性小于1%, 噪声小于0.093fC. 为了验证电子学读出系统对硅微条探测器单元的读出能力, 将两者集成在一起并测试了宇宙线缪子的能量沉积, 得到读出电子学系统的信噪比大于32, 缪子的电离损失能谱与Landau-Gaussian分布符合较好, 能够满足硅微条探测器单元读出电子学的设计要求.  相似文献   

2.
分析了低光度天文应用时CCD器件的主要噪声源的噪声特性和三种典型CCD读出信号处理方式的噪声抑制效果;提出了天文CCD读出信号的相关多次采样(CMS)处理新方法,并分析了四次采样抑制CCD读出噪声的实验结果。  相似文献   

3.
抽样选取了 2 7次上海天文台佘山站参与的天测与测地VLBI实验 ,分别进行了单次解算。通过分析解算参数随剩余钟行为和剩余大气效应分段拟合长度的变化 ,得到以下初步结论 :(1)选取不同分段拟合长度时 ,站坐标解算结果和时延残差加权均方根存在差异 ,最大分别至厘米级和数十皮秒 ,因而分段拟合长度不能随意选取。 (2 )分段拟合时段长度存在某一合理取值范围 ,它不宜过长 ,否则钟和大气的剩余效应短周期变化不能很好地模型化。为了保证待估参数解算时有足够的自由度 ,拟合时段不宜过短 ,否则将导致法方程近于或出现奇异 ,达不到较好控制噪声的效果。 (3)由于各次实验、同一次实验中的不同台站相应的钟和大气条件存在差异 ,有必要对每次实验以及每次实验中的各观测台站分别分析 ,寻找合适的分段拟合长度。这在实际操作中显然相当烦琐。 (4)一般而言 ,在剩余钟行为拟合长度缺省值 6 0min情况下 ,剩余大气效应分段拟合长度以介于 10min至 4 0min为宜 ;在剩余大气效应分段拟合长度缺省值 2 0min情况下 ,剩余钟行为分段拟合长度以介于 2 0min至 10 0min为宜  相似文献   

4.
天文用2K×2K高速CMOS相机的研制与测试结果   总被引:3,自引:0,他引:3  
高性能CMOS成像器件的技术近年来发展迅速,与长期在天文观测中占统治地位的CCD器件相比,CMOS在读出速度、功耗、空间应用的可靠性等方面具有一定的优势。为了探索CMOS成像器件在天文领域中的应用,我们以Fillfactory公司最新的高速、大面阵CMOS芯片LUPA 4000为基础,研制了一台天文相机并对其进行了测试。本文简要介绍了CMOS成像器件的概述,相机软、硬件系统的组成,以及在实验室条件下得到的读出噪声、增益、线性和增益等若干测试结果。  相似文献   

5.
张波  李金岭  王广利 《天文学报》2004,45(3):320-329
利用实测资料和模拟数据,分析了在天测与测地VLBI数据处理软件CALC/SOLVE中,剩余钟行为连续分段线性拟合的局限性和周期函数拟合的可行性.对CALC/SOLVE系统增配了周期函数拟合模块,并选取了1990年至2001年的1567次天测与测地VLBI实验,进行了剩余钟行为两种拟合模型情况下的实测资料综合解算.结果表明,在获得同等水平的时延拟合残差加权均方根(wrms)的情况下,对剩余钟行为采用周期函数拟合,使得解算参数的个数相比于连续分段线性拟合有显著减少,提高了解算的自由度.虽然在两种模型情况下的台站和射电源坐标以及地球定向参数等的解算精度无显著差异,但周期函数拟合存在可以识别的优势,85%以上的台站坐标和74%以上的源坐标以及51%以上的EOP精度均有所提高,均值分别为0.02mm、0.3μas和1.5μas.  相似文献   

6.
一种频率源噪声频谱拟合方法的研究   总被引:1,自引:0,他引:1  
在分析频率源的噪声特性的时候,经常需要由Allan方差或功率谱计算频率源的五种噪声强度系数的值,通常采用人工分析的方法,求出噪声系数,这严重阻碍了自动化处理的应用。给出的一种自动拟合算法可以满足这方面的需要。在最小均方误差意义下,这种算法能自动完成对噪声类别的判定、噪声区间的划分以及噪声系数确定,所有这些无须人工参予。最后,对模拟数据和实测的几种频率源的功率谱曲线进行拟合,实验研究的结果表明这种方法拟合的相对误差不超过11%。  相似文献   

7.
介绍了实现CCD整体平差的FORTRAN归算程序的详细流程,包括(a)数据收集、(b)预处理和(c)整体平差与结果输出共三个步骤,并给出了各步所调用的子程序名称及其功能说明。采用模拟数据对该程序进行了可靠性检验,并将该程序应用于4颗河外射电源的光学定位。结果表明, 由于利用整体平差方法参加归算的观测资料覆盖天区扩大,包含了较多的参考星,因而可以获得高于单底片归算的定位精度。  相似文献   

8.
针对多通道数字相机因信号串扰导致的输出图像重叠问题,基于自行研制的四通道CCD数字相机系统数据,对串扰系数进行了追踪测试,发现串扰系数与输入信号强度和系统读出速度有特定的规律。对于这类系统噪声类串扰,提出了一种基于定标和图像处理的串扰图像修正方法。该方法通过定标建立串扰比例系数与像素数字编码(Digital Number, DN)的关系,再由串扰通道反推被串扰通道的干扰量,通过还原算法进行系统差修正,最终消除串扰。测试结果表明,经过该方法修正后的图像,串扰程度可降至基底白噪声量级,图像质量得到大幅改善。该方法对成像系统中因硬件工艺缺陷造成的固定图案噪声的消除有显著效果,对系统噪声类干扰也有抑制作用,在实际应用中可以作为一般成像系统优化图像质量的补充。  相似文献   

9.
对历元偏差引起的伪距变化量逐项分解,总结历元偏差引起的伪距各误差项的偏差典型值,使用多项式插值法进行历元归算,并进行仿真分析,最后以星间链路体制下的星地伪距观测量为实例进行方法验证。仿真分析结果表明当数据采样间隔不大于5 min时,若选取合适的插值阶数,使用多项式插值法能得到优于1 mm的历元归算精度;实测数据结果表明基于多项式插值的历元归算方法是有效的,能够完成星间链路对地伪距观测量的历元归算需求,历元归算造成的误差远小于伪距本身的观测噪声。  相似文献   

10.
本文在分析CCD读出图像噪声的统计特性和目前CCD图像预处理的基础上,提出了对CCD读出数据的最佳化处理方法。该方法对CCD读出噪声和其它随机噪声都有较好的抑制效果,使用该方法可以从迭加有随机噪声的数据中得到信号的最佳估值,提高弱信号CCD读出图像的信噪比。  相似文献   

11.
As the areas of CCD detectors and CCD mosaics have become larger and larger,the number of readout channels in astronomical cameras has increased accordingly to keep the image readout time within an acceptable range.For the large area cameras or the mosaic cameras,the analog Correlated Double Sampling(aCDS)circuit used in traditional astronomical cameras for suppressing readout noise is difficult to integrate into the camera controllers within the constraints of the space and energy consumption.Recently,digital CDS(dCDS)technology has been developed to solve this problem,which also offers novel analysis and noise suppression methods.In this study,a mathematical model is presented to conveniently analyze the frequency characteristic of a dCDS circuit,which is then simulated by a numerical method for investigating the noise suppression capability with different sampling weights.Importantly,using this model,the extreme point with lowest readout noise can be predicted for a certain dCDS model;and for a specific CCD readout frequency,readout noise can be suppressed by selecting the proper dCDS model.A testing system is then constructed for validating the efficiency of the proposed method.  相似文献   

12.
Analytical theory is combined with extensive numerical simulations to compare different flavours of centroiding algorithms: thresholding, weighted centroid, correlation, quad cell (QC). For each method, optimal parameters are defined in function of photon flux, readout noise and turbulence level. We find that at very low flux the noise of QC and weighted centroid leads the best result, but the latter method can provide linear and optimal response if the weight follows spot displacements. Both methods can work with average flux as low as 10 photons per subaperture under a readout noise of three electrons. At high-flux levels, the dominant errors come from non-linearity of response, from spot truncations and distortions and from detector pixel sampling. It is shown that at high flux, centre of gravity approaches and correlation methods are equivalent (and provide better results than QC estimator) as soon as their parameters are optimized. Finally, examples of applications are given to illustrate the results obtained in the paper.  相似文献   

13.
Three different methods are presented to subtract thermal drifts and low-frequency noise from the signal of infrared array. The first is dead pixels with open Indium bumps, the second is reference output as implemented on the Hawaii2 multiplexer, and the third is dark pixels to emulate reference cells having a capacity connected to the gate of the unit cell field-effect transistor (FET). The third method is the most effective and yields a reduction in readout noise from15.4–9.4 erms. A novel method will be described to extend this readout technique to the Aladdin 1 K × 1 K InSb array. This revised version was published online in July 2006 with corrections to the Cover Date.  相似文献   

14.
Scientific CCDs designed in thick high resistivity silicon (Si) are excellent detectors for astronomy, high energy and nuclear physics, and instrumentation. Many applications can benefit from CCDs ultra low noise readout systems. The present work shows how sub electron noise CCD images can be achieved using digital signal processing techniques. These techniques allow 0.4 electrons of noise at readout bandwidths of up to 10?Kpixels per second while keeping the full CCD spatial resolution and signal dynamic range.  相似文献   

15.
Many different methods exist for reducing data obtained when an astronomical source is studied with a two-channel polarimeter, such as a Wollaston prism system. This paper presents a rigorous method of reducing the data from raw aperture photometry, and evaluates errors both by a statistical treatment, and by propagating the measured sky noise from each frame. The reduction process performs a hypothesis test for the presence of linear polarization. The probability of there being a non-zero polarization is obtained, and the best method of obtaining the normalized Stokes Parameters is discussed. Point and interval estimates are obtained for the degree of linear polarization, which is subject to positive bias; and the polarization axis is found.  相似文献   

16.
Once the need for an iterative procedure in order to solve the problem of the formation of spectral lines in the case of a model atom with many energy levels, the sequel is to seek for the most effective form of such an iterative scheme. It is an almost universal is assumed within all the iterative methods for the solution of those radiative transfer problems, in which the transfer equations are coupled to the state of the matter, to take as the input of each step of iterations the values of the opacity coefficients obtained as a result of the previous one. This is, for instance, the procedure used to correct the temperature in the computation of stellar atmosphere models, or that to build the -operator (either the exact or the approximated one) within the Accelerated Lambda Iteration methods. Yet, if we assume, in order to solve the multilevel line transfer problem, that at each step of iterations the line opacities are known, we can express via the statistical equilibrium equations the populations of the energy levels - and consequently the source functions of the relevant spectral lines - as a linear function of the full set of the corresponding mean intensities of the radiation field. Once such linear forms for the source functions, we are able to solve without the need of any further approximation the radiative transfer equations for are obtained lines, now linearly coupled through the above linear forms of the statistical equilibrium equations. This is achieved by means of the Implicit Integral Method that we already presented in a series of previous papers.  相似文献   

17.
Data reduction techniques published so far for the CoRoT N2 data product were targeted primarily on the detection of extrasolar planets. Since the whole dataset has been released, specific algorithms are required to process the lightcurves from CoRoT correctly. Though only unflagged datapoints must be chosen for scientific processing, some flags might be reconsidered. The reduction of data along with improving the signal‐to‐noise ratio can be achieved by applying a one dimensional drizzle algorithm. Gaps can be filled by linear interpolated data without harming the frequency spectrum. Magnitudes derived from the CoRoT color channels might be used to derive additional information about the targets. Depending on the needs, various filters in the frequency domain remove either the red noise background or high frequency noise. The autocorrelation function or the least squares periodogram are appropriate methods to identify periodic signals. The methods described here are not strictly limited to CoRoT data but may also be applied on Kepler data or the upcoming PLATO mission. (© 2015 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)  相似文献   

18.
The standard methods of the magnetic field measurement, based on an analysis of the relation between the Stokes V‐parameter and the first derivative of the total line profile intensity, were modified by applying a linear integral operator L to both sides of this relation. As the operator L, the operator of the wavelet transform with DOG‐wavelets is used. The key advantage of the proposed method is an effective suppression of the noise contribution to the line profile and the Stokes parameter V. The efficiency of the method has been studied using model line profiles with various noise contributions. To test the proposed method, the spectropolarimetric observations of the A0 star α2 CVn, the Of?p star HD 148937, and the A0 supergiant HD 92207 were used. The longitudinal magnetic field strengths calculated by our method appeared tobe in good agreement with those determined by other methods. (© 2014 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)  相似文献   

19.
The formation of Zeeman lines in Gaussian microturbulent magnetic fields is considered assuming LTE. General formulae are derived for the local mean values of the transfer matrix elements. The cases of one-dimensional (longitudinal), isotropic, and two-dimensional (transversal) magnetic microturbulence are studied in some detail. Asymptotic formulae are given for small mean as well as for small microturbulent magnetic fields. Characteristic effects of magnetic microturbulence on the transfer coefficients are: (i) the broadening of the frequency contours, although only for the case of longitudinal Zeeman effect and longitudinal magnetic microturbulence this effect can be described analogous to Doppler broadening, (ii) the appearance of a pseudo-Zeeman structure for nonlongitudinal magnetic microturbulence, (iii) the reduction of maximal values of circular polarization, and (iv) the appearance of characteristic linear polarization effects due to the anisotropy of the magnetic microturbulence.Line contours and polarization of Zeeman triplets are computed for Milne-Edddington atmospheres. It is shown that magnetic intensification due to microturbulent magnetic fields may be much more efficient than that due to regular fields. The gravity center of a Zeeman line observed in circularly polarized light remains a reasonable measure of the line of sight component of the mean magnetic field for a line strength47-1. For saturated lines, the gravity center distance depends significantly on the magnetic microturbulence and its anisotropy. The influence of magnetic microturbulence on the ratio of longitudinal field magnetographic signals shows that unique conclusions about the magnetic microstructure can be drawn from the line ratio measurement only in combination with further spectroscopic data or physical reasoning.  相似文献   

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