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基于信噪特征的X射线脉冲星信号去噪方法研究
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摘要
X射线脉冲星导航是一种新型的自主导航方式,可以为深空、近地轨道、地球同步轨道、椭圆轨道的航天器导航。X射线脉冲信号是导航的基础,客观地反映了脉冲星的辐射特征。事实上,由于多种因素的干扰导致X射线脉冲星的信号质量较差,如脉冲星与探测器距离遥远、宇宙背景复杂、强电磁干扰等因素。这些干扰不仅降低了X射线脉冲星信号的质量,而且严重影响了相位提取和导航参数的估计。因此,有效地滤除各种噪声干扰,提取高质量的X射线脉冲星信号是X射线脉冲星导航非常重要的工作之一,直接决定着X射线脉冲星定位、测速、测姿、计时的效率和精度。
     在获取X射线脉冲星信号过程中,受到各种人为或非人为的噪声干扰。由于各类噪声产生的机理不同,其统计特性和分布也有所不同,如X射线脉冲星自身周期的短期不稳定性引起的高斯噪声,光子到达的随机特性引起的泊松噪声,太阳风暴和X射线爆等现象引起的脉冲噪声等。显然,使用同一种噪声滤除方法难以滤除多种噪声的干扰。针对不同类型的噪声,利用各自不同的产生机理和分布特性分别滤除,才能达到抑制噪声干扰和提高信号质量的目的。X射线脉冲星信号的峰值、波形、脉宽等有其自身特点,X射线脉冲星的噪声滤除方法就是寻找信号和噪声的不同特征,并将其有效分开,从而实现X射线脉冲星信号的降噪。X射线脉冲星信号处理理论是一种涉及多学科的交叉的新型的研究领域,从公开文献来看,还没有利用信号与噪声的特性对X射线脉冲星信号的不同噪声采用不同方法的研究。
     本文在深入研究了X射线脉冲星导航原理的基础上,探讨了X射线脉冲星信号处理的必要性,探讨了X射线脉冲星探测系统中噪声源的特性,并根据噪声的机理和分布特性针对性地进行降噪方法的研究。利用RXTE卫星探测系统的实测数据,对降噪理论和方法进行了验证。论文取得的主要研究结果如下:
     1在分析了X射线脉冲星探测原理及工作过程的基础上,探讨在获取信号过程中由光子到达随机性和光子探测的随机性引入的泊松噪声、电子读出系统的引入的高斯噪声及电子干扰和特殊现象引入的突发脉冲噪声。通过分析各种噪声来源和特点,建立了相应的数学模型和统计特性。分析了RXTE卫星探测的X射线脉冲星信号的实测数据,深入研究了实测数据的结构、管理、数据处理和信号提取的方法,为降噪理论和方法的验证提供了可靠的数据源。
     2针对X射线脉冲星信号系统中产生的高斯噪声的问题,分析了噪声产生的机理和特征,通过对大量的数据分析表明仅依赖周期叠加方法难以快速的获取到高质量的光子脉冲轮廓信号,为此,提出了基于数据优化选择和Daubechies小波对X射线脉冲星信号的降噪方法,该方法针对于X射线脉冲星信号探测系统的复杂性和特殊性,预先滤除强噪声干扰导致信号无效或无意义的时间段,再对X射线脉冲星信号进行Daubechies小波分解,利用阈值策略滤除所含噪声。该方法通过将复杂问题简单化,不仅减轻了算法的负担,而且有效滤除了X射线脉冲星信号中存在的高斯噪声。为了兼顾降噪性能和计算复杂度,提出了提升小波的X射线脉冲星信号降噪方法。通过提升小波将复杂的小波变换简化为基本矩阵的运算,利用阈值化处理方法,滤除高斯噪声的干扰,快速地获取到高质量的光子脉冲轮廓。与传统方法相比,不仅能有效滤除噪声的干扰,还有利于资源受限的航天器的信号的处理。
     3针对X射线脉冲星信号探测系统中因光子辐射的随机性和探测器接收的随机性产生泊松噪声的问题,分析了泊松噪声产生的机理,提出了方差稳定性变换(VST)的泊松噪声抑制方法。该方法利用Haar-Fisz变换将含泊松噪声的信号进行VST变换,使得泊松噪声“漂白”为高斯白噪声,对变换后的信号阈值化处理,反变换即得到降噪后的信号。该方法间接地滤除了泊松噪声的干扰,扩展了X射线脉冲星信号的研究空间。另外,针对于方差稳定性变换不利于低强度的X射线脉冲星信号的问题,提出了一种利用Bayesian多尺度模型对X射线脉冲星信号估计的方法,该方法不需做变换直接地X射线脉冲星信号进行估计达到抑制噪声的目的。
     4针对X射线脉冲星探测系统中存在突发的脉冲噪声的问题,提出了一种基于局部的小波包变换去除脉冲噪声的新方法。根据脉冲噪声的非连续性、幅度大、不规则的特点,检测出受污染的脉冲噪声信号。在小波包域内对不同的脉冲噪声区间分别计算阈值进行降噪处理,而没被检测出脉冲噪声的信号则不做任何处理。针对在滤除脉冲噪声过程中丢失了部分X射线光子的时刻信息的问题,提出了对降噪后的脉冲噪声信号进行插值来增加各区间内光子到达的时间分辨率方法,从而实现了高质量的X射线脉冲轮廓的恢复。
X-ray Pulsar-based Navigation is a new kind of autonomous navigation technology,which has a huge potential for development of the spacecrafts in deep-space, near-earth,Geostationary orbit, and elliptic-orbit. X-ray pulsar signal is the basis of pulsar-basednavigation, which must objectively express the characteristic of pulsar. In fact, thesignal quality of X-ray pulsar is not ideal due to many reasons, such as the long distancebetween pulsars and earth, the complexity of cosmic background noise, the strongelectromagnetic interference, etc. These interferences not only decrease the quality ofsignal but also impact on the signal extraction and the estimation of navigationparameters. Therefore, extracting high-quality signal of X-ray pulsar is a very importantpre-propressing, and directly determines the efficiency and precision of position,velocity, attitude and timing.
     During the acquisition of X-ray pulsar signal, there are many kinds of artificialand non-artificial interference factors. The different mechanism of noises has differentstatistical characteristics and probability distribution. The fluctuation of period mayintroduce Gaussian noise, the stochastic of photon arrival may produce the Poissonnoise, the solar storm and X-ray storm may introduce impulsive noise. Obviously, it isdifficult to filter all kinds of noise using the same denoising method. Therefore, eachnoise properties mechanisms must be researched individually to obtain good denoisingresults. According to the characteristic of X-ray pulsar, pulse peak, pulse width, pulseprofile, the denoising method is trying to find the different characteristics betweenX-ray pulsar signal and noise, and distinguish the signal and noise to accomplish thedenoising. X-ray pulsar signal processing, as a new cross-field research field, has nospecified documents to introduce to filter the noise based on synthetic analysis of thecharacteristics of different kinds of noises.
     The importance of the X-ray pulsar signal processing is introduced on the basis ofthe navigation principle of X-ray pulsar. The characteristics of the noise sources inobserving system of X-ray pulsar are discussed. Then several denoising methods areproposed according to the mechanism and distribution of noise. The theories andmethods are verifed by the observing system RXTE. The main works can besummarized as follows.
     1Noise source and its character in observation process of X-ray pulsar signal. Theobservation principle and process are analyzed. Noises imported in X-ray pulsar acquisition, including Poisson noise caused by randomness of photon arrival anddetection, Gaussian noise caused by electronic readout and impulsive noise caused byelectrical interference and special astronomical phenomenon, are discussed. Themathematical model and statistical characteristics of the noise are established byanalyzing the source and feature of the noise. And the measured data from RXTE, thestructure, the method of signal extraction, are analyzed, which provides credible datasource for verification of the theory and method.
     2Considering Gaussian noise from the observation system of X-ray pulsar signal,the mechanism and feature of noise are analyzed. It is difficult to obtain high-qualitypulsar profile only by epoch folding. A Gaussian noise removal method based on dataoptimization and Daubechies wavelet is proposed. Considering the complexity of theobservation system for the X-ray pulsar signal, Firstly, the method selects out goodinterval from measured data, Secondly decomposes the signal by Daubechies wavelet,then filtering the Gaussian noise by threshold policy. The method, making the complexmatters easier, reduces computational complexity, but also Gaussian noise effectively.The processing platform of X-ray pulsar signal is in a resource-constrained device. Inorder to balance the complexity and performance, a denoising method based liftingscheme wavelet is proposed. The lifting scheme reduced the complex wavelettransformation to the basic matrix calculation. The SNR of pulsar profile based on thelifting scheme is improved by setting a thresholding value to removal the Gaussiannoise. The method is better for engineering implementation than the traditional one.
     3The Poisson noise introduced by the randomness of photon arrival and photondetection in observation system of X-ray pulsar signal is analyzed. Considering thePoisson property of X-ray pulsar signal, a Poisson noise suppression method based onVariance Stabilization Transform is proposed. The signal containing Poisson noise istransformed to Gaussian white noise by Haar-Fisz transformation. The noise is reducedby thresholding and inverse transform of Haar-Fisz. The indirect method filters thePoisson noise and extends the research space for X-ray pulsar signal. Besides,a methodbased on Bayesian multi-scale model is proposed by directly suppression the noiseinterference.
     4Considering impulsive noise characteristic in X-ray pulsar observation system, animpulsive noise suppression method based on wavelet packet transform is proposed.The detection algorithm named Linear Filtering could find out the peak number ofimpulsive noise by the impulsive noise characteristics, such as discontinuity, large frequency and irregulations. In wavelet packets domain, the impulsive noise overdifferent sections are filtered by thresholding policy. Especially, no noise signals doneed treatment. For the loss of time information in denoised processing, the denoisedsignal is interpolated to obtain high time resolution, which recovers a high-quanlityphoton pulsar profile.
引文
[1]J.L.LeMay. Satellite Autonomous Navigation: Status and History. Proceedings ofthe AIAA Guidance and Navigation Symposium,1986:110-121.
    [2]朱俊.基于星间链路的导航卫星轨道确定及时间同步方法研究.长沙:国防科技大学,2011.
    [3]张育林,范丽,张艳,等.卫星星座理论与设计.北京:科学出版社,2008.
    [4]帅平,李明,陈绍龙,等.X射线脉冲星导航系统原理与方法.北京:中国宇航出版社,2009.
    [5]张育林,曾国强,王兆魁,郝继刚.分布式卫星系统理论及应用.北京:科学出版社,2008.
    [6]Laurie Tetley, David Calcutt. Electronic Navigation System(3rd edition).Planta treepressce,2001.
    [7]Lamer G.,Wagner S. J. Markarian501in X-ray bright state-RXTEobservations.Astronomy and Astrophysics,1998,331:L13-L16.
    [8]Chang H.-K.,Ho C. RXTE Observation of PSR B1951+32. Astrophysical JournalLetters,1997,479:125-130.
    [9]Hewish A., S.J.Bell,J.D.Pilkington,P.F.Scott,et al.Observation of Rapidly PulsatingRadio Source.Nature,1968,217(5130):709-713.
    [10]R.A. Hulse,J.H.Taylor. Discovery of a pulsar in a binary system. AstrophysicalJournal,1975,195(2):51-53.
    [11]D.C. Backer,S.R.Kulkarni,CarL Heiles,et al.A millisecond pulsar. Nature,1982,300(5893):315-318.
    [12]孙景荣,许录平王婷.基于双谱滤波的脉冲信号消噪方法.华中科技大学学报,2010,38(8):9-12.
    [13]刘劲,马杰,田金文.基于小波和双谱的脉冲星信号识别.信息与控制,2009,38(2):249-252.
    [14]Amir Abbas Emadzadeh, Jason Speyer. Navigation in Space by X-ray Pulsars.New York: Springer,2011.
    [15]帅平,绍龙.X射线脉冲星导航技术及前景分析.中国航天,2006,1(1):27-32.
    [16]杨廷高,南仁东,金乘进等.脉冲星在空间飞行器定位中的应用.天文学进展,2007,25(3):249-261.
    [17]费保俊,孙维瑾,肖昱等. X射线脉冲星自主导航的基本测量原理.装甲兵工程学院学报,2006,20(3):59-63.
    [18]郑伟,孙守明,汤国建.基于X射线脉冲星的深空自主导航方法.中国空间科学技术,2008,28(5):1-6.
    [19]Amir A.Emadzadeh, A.Robert Golshan, Jason L.Speyer.Consistent Estimatioin ofPulse Delay For X-ray Pulsar based relation navigation.Joint48th Conference onDecision and Control and28th Chinese Control Conference,2009:1488-1493.
    [20]Tsygankov S., Lutovinov A. Churazov E., et al. Pulse profile and cyclotron lineenergy dependence on X-ray pulsars luminosity.13th Young Scientists' Conferenceon Astronomy and Space Physics,2006,115.
    [21]胡慧君,赵宝升,盛立志等.基于X射线脉冲星导航的地面模拟系统研究.物理学报,2011,60(2):029701
    [22]刘利,郑伟,汤国建,孙守明.基于X射线脉冲星的导航半实物仿真系统.国防科技大学学报,2012,34(5):10-14
    [23]李小平,谢楷,刘彦明等.具有高时频稳定度的X射线脉冲星光子信号地面模拟系统.专利号:201210245565.
    [24]胡慧君,赵宝升,盛立志等.X射线脉冲星累积脉冲轮廓泊松噪声去除的研究.光学学报,2011,31(8):0804002.
    [25]谢振华,许录平,倪广仁等.基于一维选择线谱的脉冲星辐射脉冲信号辨识.红外与毫米波学报,2007,26(3):187-195.
    [26]苏哲,许录平,王光耀等.基于离散方波变换的脉冲星微弱信号周期性检测.宇航学报,2009,30(6):2243-2248.
    [27]苏哲,王勇,许录平等.一种新的脉冲星累积脉冲轮廓辨识算法.宇航学报,2010,31(6):1563-1568.
    [28]李建勋,柯熙政,汪丽.基于高阶统计量自适应滤波的毫秒脉冲星信号处理.西安理工大学学报,2009,25(1):76-79.
    [29]胡慧君,赵宝升,盛立志等.一种基于泊松分布的提高X射线脉冲星脉冲轮廓信噪比的方法.中国科学:物理学力学天文学,2011,41:1015-1020.
    [30]E. A.Saleh, Carl Yeich Malvin.Multiplied-Poisson Noise in pulse Particle andPhoton Detection. Proceedings of the IEEE,1982,70(3):229-244.
    [31]John Hanson, Suneel Sheikh,Paul Graven,et al.Noise Analysis for X-rayNavigation Systems. Position, Location and Navigation Symposium,IEEEMonterey, CA US,2008,5:704-713.
    [32]M. A Anne,Rim Dib, Msrgaret A. Livin stone, et al. Red Noise in AnomalousX-ray Pulsar Timing Residuals.AIP Conference Proceedings,2008,983(1):265-277.
    [33]胡慧君,赵宝升,盛立志等.X射线脉冲星累积脉冲轮廓泊松噪声去除的研究.光学学报,2011,31(8):0804002.
    [34]Jean-Luc Starck, Fionn Murtagh. Handbook of Astronomical Data Analysis.Springer-Verlag Press,2010.
    [35]Eric D. Feigelson, G. Jogesh Badu.Statitical Challenges in Astronomy SpringerPress,2000.
    [36]J.V. Wall,C. R. Jenkins. Practical statistics for Astronomers. CambridgePress,2003.
    [37]Cabriel Cristobal, Peter Schelkens, Hugo Thienpont. Optical and Digital ImageProcessing. WILEY-VCH Verlag GmbH&Co,2011.
    [38]J. L. Starck, F. Muitagh. Astronomical Image and Data Analysis(2nd edition).Springer press,2006.
    [39]Galloway D. K. Spectrum and pulse profile formation in strong-field X-raypulsars.PhD Thesis, University of Tasmania, Australia,2000.
    [40]Werner Becher.Neutron Stars and Pulsars.German: Springer,2009.
    [41]Geoff McNamara. Clock in the sky-The story of Pulsar[M]. Springer Press,2008.
    [42]Walter H.G. Lewin, Michiel Van der Klis. Compact Stellar X-Ray Sources.Camberidge University Press,2006.
    [43]Steve B. Howell. Handbook of CCD Astronomy. Cambridge UniversityPress,2006.
    [44]Hannikainen Diana Carina. Multiwavelength studies of radio-jet X-ray binaries.HELSINGIN YLIOPISTO,1999.
    [45]Prith A.Arnaud, Randall K. Smith and Aneta Siemiginowska. Handbook of X-rayAstronomy.Cambridge University Press,2011.
    [46]Martin V. Zombeck. Handbook of Space Astronomy and Astrophysics. CambridgeUniversity Press,2007.
    [47]G.anab Ghosh. Rotation and Accretion Powered Pulsars. USA: World ScientificPublishing,2007.
    [48]S. S. Hasan, R. T. Gangadhara, V. Krishan. Turbulence, Dynamos, Accretion Disks,Pulsars and Collective Plasma Processes. Springer:2009.
    [49]F. P. Gavriil, V. M. Kaspi, P. M. Woods. Magnetar-like X-ray Bursts from anAnomalous X-ray Pulsar. Astrophysics. Nature,2002,astro-ph/0209202.
    [50]Ke Zschornack. Handbook of X-ray Data. Springer,2006.
    [51]James E. Mark. Methods of X-ray and Neutron Scattering in Polymer Science.Oxford University Press,2000.
    [52]http://www.atnf.csiro.au/research/pulsar/psrcat/
    [53]Wikipedians.Hadronic Matter: An overview[M].PEDIA PRESS
    [54]Chetana Jain, Biswajit Paul. Pulse Profile stability of the Crab pulsar. Research inAstron. Astrophys,2011,11(10):1134-1142.
    [55]Hambaryan V., Neuh user R., Kokkotas K. D..Bayesian timing analysis of giantflare of SGR180620by RXTE PCA. Astronomy&Astrophysics,2011,528:A45-A50.
    [56]Gangadhara R. T., Xilouris K. M., von Hoensbroech A., et al.Role of timeresolution on polarization of pulsar radiation.Astronomy and Astrophysics,1999,342:474-479.
    [57]http://heasarc.gsfc.nasa.gov/Tools/w3pimms_pro.html
    [58]Tsujimoto M., Guainazzi M., Plucinsky P. P.. Cross-calibration of the X-rayinstruments onboard the Chandra, INTEGRAL, RXTE, Suzaku, Swift, andXMM-Newton observatories using.Astronomy and Astrophysics,2011,525:A15-A30.
    [59]F. Favata, A. N. Parmar, U. Lammers, et al. The SAX-LEGSPC Data Reductionand Analysis System: An example of a Minimalist Approach. Astronmical DataAnaylsis Software and Systems IV, ASP Conference Series,1995,70:383-386.
    [60]Kinzer R. L., Jung G. V., Gruber D. E., et al.Diffuse Cosmic Gamma RadiationMeasured by HEAO1. Astrophysical Journal,1997,475:361-367.
    [61]Cominsky L., Roberts M., Lee A., et al.HEAO A-1Archival Observations ofGalactic X-Ray Binaries.American Astronomical Society,184th AAS Meeting,#09.07; Bulletin of the American Astronomical Society,1994,26:872.
    [62]Collmar Werner. Analysis of an observation of the X ray astronomy satelliteEXOSAT at the low mass X ray binary star system GX5-1. Ph.D. Thesis TuebingenUniv.,1988.
    [63]Oegelman Hakki; Hasinger Guenther. Period measurements of the50millisecondpulsar PSR0540-69with the EXOSAT satellite.AstrophysicalJournal,1990,353(2):21-23.
    [64]Voges W.,Aschenbach B., Boller Th., et al.The ROSAT all-sky survey brightsource catalogue.Astronomy and Astrophysics,1999,349:389-405.
    [65]Ledlow Michael J., Voges Wolfgang, Owen Frazer N., et al. The X-Ray Propertiesof Nearby Abell Clusters from the ROSAT All-Sky Survey: The Sample andCorrelations with Optical Properties. The Astronomical Journal,2003,126(6):2740-2751.
    [66]Appenzeller I.,Zickgraf F.-J., Krautter J., et al.. Identification of a complete sampleof northern ROSAT all-sky survey X-ray sources. VII. The AGNsubsample.Astronomy and Astrophysics,2000,364:443-449.
    [67]Reba M. Bandyopadhyay, K. S. Wood, P. Hertz, et al. Observations of GRS1915+105from the USA Experiment on ARGOS. Astrophysics and SpaceScience,2001,276:23-24.
    [68]SHAPOSHNIKOV N. V., K. M. JAHODA, C. B. MARKWARDT, et al.ADVANCES IN THE RXTE PROPORTIONAL COUNTER ARRAYCALIBRATION: NEARING THE STATISTICAL LIMIT. AstrophysicalJournal,2012,757:159-175.
    [69]Tadayuki Takahashi, Yasunobu Uchiyama, Lukasz Stawarz.MultiwavelengthAstronomy and CTA: X-rays.Astrtopartical Physics,2013,43:142-154.
    [70]Furst Felix, Wilms Jorn, Rothschild Richard E.. et al. Temporal variations ofstrength and location of the South Atlantic Anomaly as measured by RXTE.Earthand Planetary Science Letters,2009,281(3):125-133.
    [71]D.E. Gruber, D. MacDonald, R.E. Rothschild. Granularity of the DiffuseBackground Observed. Nuclear Physics,1998,69(1):625-628.
    [72]Giacconi Riccardo, Zirm Andrew,Wang JunXian, et al..Chandra Deep Field South:The1Ms Catalog.The Astrophysical Journal Supplement Series,2002,139(2):369-410.
    [73]Muno M. P., Baganoff F. K., Bautz M. W., et al.Diffuse X-Ray Emission in a DeepChandra Image of the Galactic Center.The AstrophysicalJournal,2004,613(1):326-342.
    [74]Muno M. P., Baganoff F. K.,Bautz M.W.,et al.A Deep Chandra Catalog of X-RayPoint Sources toward the Galactic Center.The AstrophysicalJournal,2003,589(1):225-241.
    [75]Iwan D., Shafer R.A., Marshall F. E.. A large scale height galactic component ofthe diffuse2-60keV background.Astrophysical Journal,1982,260(1):111-123.
    [76]Sazonov S.,Revnivtsev M., Gilfanov M.,Churazov E.,et al..X-ray luminosityfunction of faint point sources in the Milky Way.Astronomy and Astrophysics,2006,450(1):117-128.
    [77]Revnivtsev M., Sazonov S., Jahoda K., et al.RXTE all-sky slew survey. Catalog ofX-ray sources at|b|>10.Astronomy and Astrophysics,2004,418:927-936.
    [78]H. M. Horstman, G. Cavallo, E. Moretti-Horstman.The X and γ diffuse background.La Rivista del Nuovo Cimento,1975,5(2):255-311.
    [79]S.L. Snowden, M.J. Freyberg, P.P. Plucinsky, et al.First Maps of the Soft X-rayDiffuse Background from the ROSAT XRT/PSPC All-Sky Survey.AstrophysicalJournal,1995,454:643-653.
    [80]Warwick R. S., Norton A. J.,Turner M. J. L., et al. A survey of the galacticplane with EXOSAT. Monthly Notices of the Royal AstronomicalSociety,1988,232:551-564.
    [81]Revnivtsev M.Distribution of the Galactic bulge emission at|b|>2o according tothe RXTE Galactic Center scans.Astronomy and Astrophysics,2003,410:865-870.
    [82]Valinia Azita, Marshall Francis E. RXTE Measurement of the Diffuse X-RayEmission from the Galactic Ridge: Implications for the Energetics of theInterstellar Medium.The Astrophysical Journal,1998,505(1):134-147.
    [83]A.J. Barger.The X-ray Background. RevMex AA(Serie de Conferencias),2003,17:226-229.
    [84]M. Revnivtsev, S. Sazonov, M. Gilfanov, et al. Origin of the Galactic ridge X-rayemission. Astronomy&Astrophysics,2006,452:169-178.
    [85]M. Markevitch, M. W. Bautz,B. Biller, et al.. CHANDRA SPECTRA OF THESOFT X-RAY DIFFUSE BACKGROUND. The Astrophysical Journal,2003,583:70–84.
    [86]Worrall D. M., Marshall F.E., Boldt E.A., et al.. HEAO1measurements of thegalactic ridge. Astrophysical Journal,1982,255(1):111-121.
    [87]Giacconi Riccardo, Gursky Herbert, Paolini Frank R., et al..Evidence for x RaysFrom Sources Outside the Solar System.Physical ReviewLetters,1962,9(11):439-443.
    [88]Worrall, D. M.,Marshall, F.E.. Stellar contributions to the hard X-ray galactic ridge.Astrophysical Journal,1983,267:691-697.
    [89]Ottmann R.,Schmitt J.H.M.M..The contributions of RSCVn systems to the diffuseX-ray background.Astronomy and Astrophysics,1992,256(2):421-427.
    [90]Koyama K.,Makishima K., Tanaka, Y., et al. Thermal X-ray emission with intense6.7-keV iron line from the Galactic ridge.Astronomical Society of Japan,1986,38(1):121-131.
    [91]Mukai K., Shiokawa K. The EXOSAT Medium Energy (ME) Sample of DwarfNovae. Astrophysical Journal,1993,418:863-873.
    [92]Martijn de Kool, Ulrich Anzer. A simple analysis of period noise in binary X-raypulsars. Royal Astronomical society,1993,262:726-734.
    [93]Falanga M. Modelling the outburst profile of X-ray millisecond pulsars.ADECADE OF ACCRETING MILLISECOND X-RAY PULSARS. AIP ConferenceProceedings,2008,1068:103-114.
    [94]Sabat Hanna A. Using Astrophysical Data Archives In Astrophysical Research:RXTE As A Case Study. Astrophysics and Space Science,2000,273(4):141-153.
    [95]Pesquet J., Krim H.,Leporini D., et al.. Bayesian approach to best basis selection.Acoustics, Speech, and Signal Processing,1996. ICASSP-96. ConferenceProceedings.,1996IEEE International Conference on,1996,5:2634-2637.
    [96]Mallat S, Hwang W L. Singularity detection and processingwith wavelet IEEETrans.on InformationTheory,1992,38(2):617-693
    [97]Goddard Space Flight Center. HEAdas Developer's Guide,USA,2008.http://heasarc.gsfc.nasa.gov/docs/software/lheasoft/HEAdas_Developer's_Guide.pdf
    [98]J. W. Lewis. Cheating Poisson: A Biased Method for Detecting Faint Sources inAll-Sky Survey Data. Astronomical Data Analysis Software and Systems IV, ASPConference Series,1995,77:20-25.
    [99]D. A. Leahy. Searches for pulsed emission: improved determination of Period andamplitude form epoch folding for sinusoidal signals. Astronomy and Astrophysics,1987,180:275-277.
    [100]D. A. Leahy, R.F. Elsner, M. C. Weisskopf. On searchs for Periodic PulsedEmission: The Rayleigh Test Compared to Epoch Folding. The AstrophysicalJournal,1983,272:256-258.
    [101]S. Larsson. Parameter estimation in epoch folding analysis. Astron. Astropyhs.Suppl. Ser,1996,117:197-201.
    [102]Shaw R A, Payne H E, and Hayes J E. The SAX-LEGSPC data reduction andanalysis system: an example of a minimalist approach. Astronomical Data AnalysisSoftware and Systems IV, Baltimore, Maryland, USA, September25-28,1995.
    [103]王志武,丁国清,颜国正等,自适应提升小波变换与图像去噪.红外与毫米学报,2002,21(6):447-450.
    [104]W Sweldens.The lifting scheme:A new philosophy in biorthogonal waveletconstruction. Proc SPIE,1995,25(1):68-79.
    [104]I Daubechies, W Swenldens. Factoring wavelet transform into lifting steps. J.Fourier Anal. Appl.,1998,4(3):247~269
    [106]邵永社,李晶,何向晨等.提升小波与隐马尔科夫模型的SAR图像噪声滤波.系统工程与电子技术,2008,30(6):828831
    [107]Nan Nasri, H. Nezamabadi-pour. Image denoising in the wavelet domain using anew adaptive thresholding function [J].Neurocomputing,2009,72(4):1012~1025
    [108]F. Favata, A. N. Parmar, U. Lamers et al. The SAX-LEGSPC Data Reduction andAnalysis System: an Example of a Minimalist Approach. Astronomical DataAnalysis Software and Systems IV,1995,77:383
    [109]李学锋,权赫. Daubechies小波函数特征对MRTD算法的影响性分析.宇航学报,2011,32(11):3239-3244.
    [110]刘云侠,杨国诗,贾群.基于双提升小波的自适应混沌信号降噪.电子学报,2011,39(1):13~17
    [111]X.-P. Zhang, M.D. Desai. Addaptive denoising based on SURE risk, IEEE SignalProcess. Lett.1998,5(10):265~267
    [112]X.-P. Zhang. Thresholding neural network for adaptive noise reduction. IEEETrans. Neural Networks,2001,12(3):567~584
    [113]Sheikh I S. The use of variable celestial X-ray sources for spacecraft navigation.Maryland: University of Maryland,2005.
    [114]Anscombe F.The transformation of Poisson binomial and negative binomialdata[J].Biometrika,1948,35(1):246-254
    [115]Fisz,M. The limiting distribution of a function of two independent variables andits statistical application. Colloquium Mathematicum,1955,3:138–146
    [116]Kolaczyk, E.D., D.D. Dixon. Nonparametric estimation of intensity maps usingHaar wavelets and Poisson noise characteristics. The AstrophysicalJournal,2000,534(1):490-505.
    [117]Zhang B., J.M. Fadili, J-L. Starck. Wavelets, ridgelets, and curvelets for Poissonnoise removal. IEEE Trans. Image Process.,2008,17(7):1093-1108.
    [118]Zachary T. Harmany, Roummel F. Marcia, Rebecca M. Willett. This isSPIRAL-TAP: Sparse Poisson Intensity Reconstruction Algorithms-Theory andPractice. IEEE TRANSACTIONS ON IMAGE PROCESSING,2012,21(36):1084-1096.
    [119]孙景荣,许录平,王婷.一种用于脉冲星信号去噪的新方法.西安电子科技大学学报,2010,37(6):1059-1064.
    [120]D.L. Donoho, R.R. Coifman. Translation-Invariant Denoising. Wavelets andStatistics,1995,125:1-26.
    [121]Curtiss, J.H.. On transformations used in the analysis of variance. The Annals ofMathematical Statistics,1943,14(2):107-122.
    [122]Markku M, Alessandro F. Optimal inversion of the Anscombe transformation inlow-count Poisson image denoising.IEEE TRANSACTIONS ON IMAGEPROCESSING,2011,20(1):99-108.
    [123]D.L. Donoho. Non-linear wavelet methods for recovery of signals, densities andspectra from indirect and noisy data. American MathematicalSociety,1993,47:173–205.
    [124]Makitalo M., A. Foi. On the inversion of the Anscombe transformation inlow-count Poisson image denoising,Proc. Int. Workshop on Local and Non-LocalApprox. in Image Process., LNLA2009,26-32.
    [125]Piotr Fryzlewicz. Haar-Fisz methodology for interpretable estimation of large,sparse, time-varying volatility matrices. Hernando: UNIVERSITE CATHOLIQUEDE LOUVAIN,2011.
    [126]Fryzlewicz, P., and G.P. Nason, ìA Haar-Fisz Algorithm for Poisson In-tensityEstimation, Journal of Computational and Graphical Statistics,2004,13(3):621-638.
    [127]Kolaczyk, E.D. Bayesian Multi-Scale Models for Poisson Processes. Journal ofthe American Statistical Association,1999,94(447):920-933.
    [128]胡慧君,赵宝升,盛立志等.一种基于泊松分布的提高X射线脉冲星脉冲轮廓信噪比的方法.中国科学:物理学力学天文学,2011,41:1015-1020.
    [129]R.D. Blandford, A.Hewish, A. G.Lyne, et al. Pulsars as Physics Laboratories.The Royal Society Oxford University Press,1993.
    [130]Lefkimmiatis, S., P. Maragos, G. Papandreou. Bayesian inference on multiscalemodels for Poisson intensity estimation: Applications to photon-limited imagedenoising. IEEE Trans. Image Process.,2009,18(8):1724-1741.
    [131]Chipman H.A.,Kolacxyk, E.D.,McCulloch, R.E..Signal de-noising using adaptiveBayesian wavelet shrinkage. Time-Frequency and Time-Scale Analysis,1996.,Proceedings of the IEEE-SP International Symposium on,1996,1(1):225-228.
    [132]Huang X.,Madoc, A.C., Cheetham A.D.. Wavelet-based Bayesian estimator forPoisson noise removal from images.Multimedia and Expo,2003. ICME '03.Proceedings.2003International Conference on,2003,1:593-596.
    [133]Box G.E.P., Cox D.R.. An analysis of transformations. J. Roy. Stat. Soc. Series B(Methodological),1964,26:211-252.
    [134]Markku MAkitalo,Alessandro Foi. A Closed-Form Approximation of the ExactUnbiased Inverse of the Anscombe Variance-Stabilizing Transformation.IEEETRANSACTIONS ON IMAGE PROCESSING,2011,20(9):2697-2680.
    [135]B.P. Durbin, J.S. Hardin, D.M. Hawkins, et al. A variance-stabilizingtransformation for gene-expression microarray data. BIOINFORMATICA.2002,18(1):105-110.
    [136]Kolaczyk, E. D..Bayesian multiscale models for Poisson processes. J. Amer.Statist. Ass.,1999,94:920–933
    [137]Peter Congdon. Bayesian Statistical Modeling(2nd edition). Willey,2006.
    [138]Rebecca M. Willett, Robert D. Nowak. Multiscale Poisson Intensity and DensityEstimation.IEEE TRANSACTIONS ON INFORMATION THEORY,2007,53(9):3171-3189.
    [139]D.L. Donoho, N. Dyn, D. Levin. Smooth Multiwavelet Duals of Alpert Bases byMoment-Interpolation, with Applications to Re-cursive Partitioning, Applied andComputational Harmonic Analysis,2000,9:166–203.
    [140]Andrew Gelman, John B. Carlin, Hal S. Stern. Bayesian data analysis (2ndedition),2003.
    [141]J. Berger, S. Fienberg, J. Gani, et al. Bayesian Spectrum Analysis and ParameterEstimation. Springger-Verlag,1997.
    [142]James O. Berger. Statistical Decision Theory and Bayesian Analysis (2nd edition).Springer-Verlag,1985.
    [143]Junko Murakami. Bayesian Posterior Mean Estimates for Poisson HiddenMarkov Models. Computational Statistics&Data Analysis,2009,53(4):941-955.
    [144]Donoho D L, Johnstone I M.Ideal spatial adaption by wavelet shrinkage.Biometrika.Biometrika,1994,81(1):425-455
    [145]NASON G P, Rainer V S. Wavelet shrinkage using cross-validation. Journal ofthe Royal Statistical Society,Series B.Journal of the Royal Statistical Society,SeriesB,1996,58(1):463-479
    [146]Baraniuk R G. Optimal tree approximation with wavelets.Wavelet applications insignal and image processing VII,Proc. SPIE,1999,3813:206-214
    [147]Leonard Parker, Jonathan Z. Simon. Einstein equation with quantum correctionsreduced to second order. Physical Review D,1993,47(4):1339-1355.
    [148]Fairhead L.,Bretagnon P.. An Analytic Formula for the Time TransformationTB-TT.Astronomy and Astrophysics,1990,229(1):240-247.
    [149]Irwin A.W., Fukushima T.. A Numerical Time Ephemeris of the Earth. AstronomyAnd Astrophysics,1999,8(348):642-652.
    [150]T. Baumgarte, S. Shapiro. Numerical integration of Einstein's field equations.Phys. Rev. D,1999,59:024007.
    [151]T. Baumgarte, G. Cook, M. Scheel, et al. Binary Neutron Stars in GeneralRelativity: Quasiequilibrium Models. Phys. Rev. Lett.1997,79:1182-1185.
    [152]Nipuni Palliyaguru, Maura McLaughlin, Evan Keane. Radio Properties ofRotating Radio Transients I: searches for periodicities and randomness in pulsearrival times.Mon. Not. R. Astron. Soc.2011,521(1):1-11.
    [153]M. Kramer, A.G. Lyne, J.T. O'Brien, et al. A periodically active pulsar givinginsight into magnetospheric physics.Science,2006,312:549-551.
    [154]Camilo F. Pulsar Period and Magnetic Field Evolution. Astronomical Society ofthe Pacific Conference Series,1996,105:39-47.
    [155]N. D’Amico, B.W. Stappers, M. Bailes, et al. The Parkes Southern Pulsar Survey–III. Timing of long Period Pulsars. Monthly Notices,1998,297(1):28-40.
    [156]Kolaczyk E.D., Non-Parametric Estimation of Gamma-Ray Burst IntensitiesUsing Haar Wavelets. The Astrophysical Journal,2000,483:340-349.
    [157]ShP. Barbieri, R.E. Mahmot. October-November2003’s space weather andoperations lessons and learned. SPACE WEATHER,2004,2(9): S09002.
    [158]N. Gopalswamy. Interplanetary acceleration of coronal mass ejections.Geophysical Research letters,2012,27(2):.
    [159]P.SREEKUMAR, D.L. BERTSCH,B. L. DINGUS,et al.EGRET Observations ofthe Extragalactic Gamma-Ray Emission.THE ASTROPHYSICALJOURNAL,1998,494:523-534.
    [160]Zdziarski Andrzej A.,Johnson W. Neil,Done Chris, et al.The averageX-ray/gamma-ray spectra of Seyfert galaxies from GINGA and OSSE and theorigin of the cosmic X-ray background. Astrophysical Journal,1995,438(2):63-66.
    [161]Comastri A., Setti G.,Zamorani G., et al.The contribution of AGNs to the X-raybackground. Astronomy and Astrophysics,1995,296:1-22.
    [162]Leiter Darryl, Boldt Elihu. Spectral-luminosity evolution of active galactic nuclei(AGN). Proceedings of the2nd Annual Topical Astrophysics Conference,AIPConference Proceedings,1991,254:370-373.
    [162]Zdziarski Andrzej A. Contributions of AGNs and SNe IA to the cosmic X-ray andgamma-ray backgrounds. Monthly Notices of the Royal Astronomical Society,1996,281:9-15.
    [164]David F. Webb, Joe H. Allen. Spacecraft and Ground Anomalies Related to theOctober-November2003Solar Activity. SPACE WEATHER,2004,2(3):SW000075
    [165]Uwe Oberlack.Viewpoint: Extragalactic diffuse gamma-ray emission at highenergies. American Physical Society,2010,3(21):1-3
    [166]Smith Donald Andrew. Observations of x-ray counterparts to gamma-ray burstsin RXTE's all-sky monitor.MASSACHUSETTS INSTITUTE OFTECHNOLOGY,1999.
    [167]Bradt H. V., Smith D. A.Gamma-ray burst positions from the ASM on RXTE.Astronomy and Astrophysics Supplement,1999,138:423-424.
    [168]Zamorano J., Rego M., Gallego J. G., et al.Survey of emission-line galaxies:Universidad Complutense de Madrid list. Astrophysical Journal SupplementSeries,1994,95(2):387-399.
    [169]Uttley P., McHardy I. M., Papadakis I. E.. Measuring the broad-band powerspectra of active galactic nuclei with RXTE. Monthly Notices of the RoyalAstronomical Society,2002,332(1):231-250.
    [170]Bikmaev I. F., Sunyaev R. A., Revnivtsev M. G.,et al..New nearby active galacticnuclei among INTEGRAL and RXTE X-ray sources. Astronomy Letters,2006,32(4)221-227.
    [171]L. Boirin, L. Keek, M.Mendez, et al. Discovery of X-ray burst triplets in EXO0748-676. Astronomy&Astrophysics,2007,465(2):559-573.
    [172]S.E. Woosl ey,A. Heger,A. Cummi ng, et al.MODELS FOR TYPE I X-RAYBURSTS WITH IMPROVED NUCLEAR PHYSICS.The Astrophysical JournalSupplement Series,2004,151:75-102.
    [173]J. J. M. int Zand, D. K. Galloway, H. L. Marshall, et al.A bright thermonuclearX-ray burst simultaneously observed with Chandra and RXTE.Astronlmy&Astrophysics,2013,553:11-20.
    [174]Hauke Worpel, Duncan K. Galloway,Daniel J. Price. EVIDENCE FORACCRETION RATE CHANGE DURING TYPE I X-RAY BURSTS.TheAstrophysical Journal,2013,772(2):1-15.
    [175]解妍琼.太阳风暴的综合研究.中国科学院研究生院博士学位论文,2007.
    [176]A.R. KING, U. KOLB.The Formation of Low-Mass Transient X-RayBinaries.THE ASTROPHYSICAL JOURNA,1997,481:918-925.
    [177]贺昊宁.伽马射线暴多信使手段的研究.南京大学博士学位论文,2012.
    [178]Chelovekov I. V., Lutovinov A. A., Grebenev S. A.,et al. Observations of theX-ray Burster MX0836-42by the INTEGRAL and RXTE Orbiting Observatories.Astronomy Letters,2005,31(10):681-694.
    [179]孔思伟.伽马暴余辉及伽马射线脉冲双星多波段辐射的研究.南京大学博士学位论文,2012.
    [180]D. N. Burrows.Bright X-ray Flares in Gamma-Ray Burst Afterglows. Science,2005,309(5742):1833–1835.
    [181] J.A. Nousek. Evidence for a Canonical Gamma-Ray Burst Afterglow LightCurve in the Swift XRT Data.2006,Astrophysical Journal642:389–400.
    [182]谭颖.活动星系核的X射线观测研究.中国科学技术大学博士学位论文,2012.
    [183]MacDonald Daniel Rufus. Measuring the granularity of the diffuse hard X-raybackground.UNIVERSITY OF CALIFORNIA, RIVERSIDE,1999.
    [184]Bachelorarbeit, vorgelegt von, Natalie Hel. The Evolution of the South AtlanticAnomaly Measured by RHESSI.Erlangen Centre for Astroparticle Physics,2010
    [185]Stefano Casadioa,Olivier Arinob. Monitoring the South Atlantic Anomaly usingATSR instrument series. Advances in Space Research,2011,48(6):1056-1066.
    [186]McFeeC. Radiation shielding considerations for the Solar-B EIS CCDs-initialdiscussion. EIS-CCD-desnote-003,1999
    [187]Furst Felix, Wilms Jorn,Rothschild Richard E,et al. Temporal variations ofstrength and location of the South Atlantic Anomaly as measured by RXTE.Earthand Planetary Science Letters,2009,281(3):125-133.
    [188]Pu Z.Y., Xie L., Jiao W.X., et al. Drift shell tracing and secular variation ofinner zone high energy proton environment in the SAA. Advances in SpaceResearch36,1973–1978,2005.
    [189]Stefano A., P.White,W.Collis.Training methods for image noise level estimationon wavelet components.Eurasip Journal on Applied SignalProcessing.2004,16:2400–2407.
    [190]张旭明,徐滨士,董世运等.去除脉冲噪声的自适应开关中值滤波.光电工程,2006,3(6):78-82.
    [191]Riji R, Keerthi A S Pillai, Madhu S. Nair, et al. Fuzzy Based DirectionalWeighted Median Filter for Impulse Noise Detection and Reduction. Fuzzy Inf.Eng.,2012,4:351-369.
    [192]Minh N. Do,Martin Vetterli. Contourlets: A Directional Multiresolution ImageRepresentation. Proc. of IEEE International Conference on Image Processing.Rochester,IEEE,2002:357-360.
    [193]S. V. Vaseghi, P. J. W. Rayner. Detection and suppression of im-pulse noise inspeech communication systems.IEE Proceedings,1990,13(1):1-10.
    [194]Sheena Govindan,S.Saravanakumar.Removal of Impulse Noise using NoiseAdaptive Fuzzy Switching Median Filter.International Conference on VLSI,Communication&Instrumentation (ICVCI)2011International Journal ofComputer Applications,2011,39-45.
    [195]Suganya C.,Umamaheswari O.Image restoration using noise adaptive fuzzyswitching weighted median filter for the removal of impulse noise. DefenseScience Research Conference and Expo (DSR),2011,1-4.
    [196]Umesh Ghanekar, Awadhesh Kumar Singh, Rajoo Pandey.A ContrastEnhancement-Based Filter for Removal of Random Valued Impulse Noise.IEEESIGNAL PROCESSING LETTERS,2010,17(1):47-50.
    [197]C. Chandra, M. S. Moore, S. K. Mitra. An ef ficient method for the removal ofimpulse noise from speech and audio signals. Proceedingsof ISCAS1998,4(1):206-208.
    [198]Lee C S, Guo S M, Hsu C Y. A novel fuzzy filter for impulse noise removal.Lecture Notes in Computer Science,2004:375-380
    [199]Schulte S, de Witte V, Nachtegael M, et al.. Fuzzy random impulse noisereduction method. Fuzzy Sets and Systems207,158(3):270-283
    [200]Petrovic N I, Crnojevic V. Universal impulse noise filter based on geneticprogramming. IEEE Transactions on Image Processing,2008,17(7):1109-1120.
    [201]Dong Y, Xu S. A new directional weighted median filter for removal ofrandom-valued impulse noise. IEEE Signal Processing Letters,2007,14(3):193-196
    [202]Hussain A, Jaffar A, Mirza A M. Detail preserving fuzzy filter for impulse noiseremoval.International Journal of Innovative Computing, Information and Control,2009,5(10(B)):3583-3591
    [203]Schulte S, Nachtegael M, de Witte V, et al.. A fuzzy impulse noise detection andreduction method. IEEE Trans. on Image Processing,2006,15(5):1153-1162.
    [204]Taam Ronald E., Chen Xingming, Swank Jean H.Rapid Bursts from GRS1915+105with RXTE.Astrophysical Journal Letters,1997,485:L83-L89.
    [205]Smith D. A., Levine A., Bradt H., et al..X-Ray Light Curves of Gamma-RayBursts Detected with the All-Sky Monitor on RXTE. The Astrophysical JournalSupplement Series,2002,141(2):415-428.
    [206]Lutovinov A. A., Revnivtsev M. G. RXTE Observations of the Transient SourcesIGR J17091-3624and IGR J18539+0727. Astronomy Letters,2003,29:719-723.
    [207]Coifman R.R., Wickerhauser M.V..Entropy-based algorithms for best basisselection. Information Theory, IEEE Transactions on,1992,38(2):713-718.
    [208]Rachel E. Learned, Alan S. Willsky. A Wavelet Packet Approach to TransientSignal Classification. Applied and Computational Harmonic Analysis,1995,2:265-278.

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