共查询到20条相似文献，搜索用时 500 毫秒
1.
菲索型光干涉望远镜得到高分辨率成像的关键是消除各子镜之间相位平移误差。宽光谱条纹对比度检测法是一种检测相位平移误差的有效办法。基于物理光学的基本原理,论证了平移误差与系统点扩展函数的关系,进而仿真了共相远场条纹像,分析了共相检测与控制过程和数据预处理的方法,提出了加权对比度的算法和共相维持的方法,最终得到了共相远场像,并与仿真结果进行了对比。结果表明,实验与仿真的共相远场像能量分布形态以及数值都比较接近,该方法可以实现对子镜之间相位平移误差的检测与控制。 相似文献
2.
闭合相位技术、U -V覆盖技术和像重构技术是光学综合孔径干涉成像的三个关键技术。文中简要介绍了光学综合孔径技术的发展历史、这三种关键技术和光学综合孔径望远镜阵的构成 ,对之进行了多光束干涉的计算机仿真和实验仿真 ,两者结果一致说明了光学综合孔径干涉成像技术中有关干涉的理论的正确性 ,指出了下一步的研究方向。 相似文献
3.
邱育海 《中国科学院上海天文台年刊》1995,(16):280-281
本文描述了密云综合孔径射电望远镜的相加系统，以及该系统将被应用于行星际闪烁观测、脉冲星观测、一维太阳高速扫描和射电源定标等工作。 相似文献
4.
《天文研究与技术》2016,(3)
利用组成星座的小卫星,分别携带分离的子望远镜和合光成像望远镜,构成Fizeau型光学综合孔径干涉系统,实现高分辨率的面源目标成像是当前的研究热点之一。这种光干涉成像系统,由于稀疏度较大,UV覆盖不全,即空间频率采样不连续,表现为系统光学传递函数有零值存在。要克服UV覆盖不全的影响,获得等效的大孔径望远镜成像效果,需要改变子孔径的空间排布,获得不同基线条件下的图像,进行空间频率信息的提取和合成,最后采用逆滤波的方法达到提高图像质量的目的。在分析单子孔径传递函数与系统传递函数关系的基础上,优化子孔径的排布方式,采用不同的频域滤波器将不同基线获得的图像中信噪比高的频率区域提取出来进行合成,再变换到空域并进行逆滤波处理,得到改善的合成图像。仿真结果显示,当得到的干涉图信噪比较低时,该方法可以有效地提高合成图像的质量。 相似文献
5.
波前检测是天文望远镜自适应光学中的重要环节。四棱锥作为一种新型的波前检测元件,与其他传统的波前传感器相比,具有较高的灵敏度。特别是对于光干涉或拼接镜面望远镜而言,四棱锥波前传感器能够被用来检测子望远镜或子镜面之间的相对光程差,从而为干涉(或共相)的实现提供有效的检测信号。在分析四棱锥波前检测原理的基础上,阐述了单孔径条件下波前倾斜检测及双孔径干涉条件下相对光程差检测的软件仿真设计和阶段性成果,并简述了下一阶段的研究计划。 相似文献
6.
南京大学太阳塔CCD成像光谱观测系统和初步观测结果 总被引：1，自引：0，他引：1
本文介绍南京大学太阳塔的ＣＣＤ成像光谱观测系统的结构，工作方式，给出了该系统的一些性能测试结果，作为应用该系统的实例，文中给出了根据该系统观测的二维光谱资料，经处理得到的一个Ｈａ耀斑在线心和不同偏带处单色像的变化过程，该耀斑的亮度场轮廓图和速度场轮廓图。 相似文献
7.
8.
回顾了光干涉与综合孔径技术发展的历史和现状，分析了国际上用于天文观测的一些著名地基和空基光干涉仪的技术特点，介绍了光干涉与综合孔径技术的发展，以及在光学综合孔径技术领域所发展的光纤与集成光学等新技术，简要介绍了近年来我国开展光干涉与综合孔径技术的进展情况。针对光干涉与综合孔径技术的发展前景和国内外技术发展趋势，发出了加快发展我国光干涉与综合孔径技术的呼吁。 相似文献
9.
《天文研究与技术》2021,(4)
为进一步提高现有实时幸运成像系统的实时性,针对第二代通用串行总线(Universal Serial Bus 2.0, USB2.0)接口的电子倍增电荷耦合(Electron Multiplying Charge-Coupled Devices, EMCCD)相机进行幸运成像观测的情况,提出了一个基于USB2.0总线数据侦听的实时幸运成像技术方案,进行了侦听电路的硬件设计和数字逻辑设计,搭建了一个具有实时侦听、传输、处理、动态更新和显示的幸运成像系统。当相机拍摄天文图像并与个人计算机(Personal Computer, PC)进行数据交互时,系统的USB2.0总线数据侦听子系统就会对交互的USB2.0总线实现无侵入式侦听,并且加以分析处理后,只将有效的天文图像数据发送给底层现场可编程门阵列(Field Programmable Gate Array, FPGA)开发板中的幸运成像子系统,然后幸运成像子系统对接收的数据进行预处理、动态选图、实时配准和叠加处理,最后采用9个实时分割阈值水平切割高分辨率图像并对二值图像进行动态更新和显示。实验结果表明,所实现的系统能够对在USB2.0总线上连续传输的10 000帧512×512像素的图像进行实时侦听、幸运成像和动态更新显示,实现了幸运成像技术的实时化。 相似文献
10.
《中国科学院上海天文台年刊》2004,(1)
望远镜监控系统可以用来监控诸如机场上空的鸟群、低空云层以及跑道和停机坪上的异常物体等机场远距离目标。整个系统的设计分为光学与机械、望远镜控制、以及监控成像与图像处理三个子系统。在光学与机械部分 ,着重论述望远镜的光学特性和电机驱动方式下的机械结构改进 ;在望远镜控制部分 ,分析了控制电机的选择、单片机的控制方式、以及计算机控制软件的功能设计 ;最后概述了监控成像与图像处理部分的初步实现方式。 相似文献
11.
Sylvie Jancart Anne Lemaitre Vincent Letocart 《Celestial Mechanics and Dynamical Astronomy》2003,86(4):363-383
Interested in the role of the inclination in our results (Jancart and Lemaitre, 2001), we analyze the process of resonance trapping due to general dissipation forces in the frame of the spatial restricted three body problem and in the case of external mean motion resonances. We compute our simulations by using the three-dimensional Extended Schubart Averaging integrator developed by Moons (1994) for all mean motion resonances. We complete it by adding the averaged contributions of general dissipative forces like Murray has proposed in the article (1994). The behavior of the inclination is especially pointed out. 相似文献
12.
本文叙述了度盘偏斜现象及其对读数显微镜Reticon比例尺测定值的影响 ,分析了产生度盘偏斜的原因和修正方法 ,文章讨论了是否需要对比例尺加上与天顶距有关的修正项问题 ,结论是只要把度盘偏心控制在 5μm以内 ,就不必加改正。 相似文献
13.
For the many-body problem in the field of general attraction, the evolution of the moment of inertia is studied, we obtain the bifurcation curves between the attainable domain and the forbidden domain in the plane (,t), where is the mean quadratic distance (proportional to the square root of the moment of inertia). That is an extension of the conclusion in [1]. Moreover, the dependence of the bifurcation curves on the generalized potential is obtained.This project is supported by the National Science Foundation of China. 相似文献
14.
M.S. Kovner V.V. Lebedev T.A. Plyasova-Bakounina V.A. Troitskaya 《Planetary and Space Science》1976,24(3):261-267
The generation of low-frequency waves in the solar wind by the flux of protons accelerated in the magnetosheath is considered. It is shown that pulsations are produced in two partly overlapping frequency ranges. The growth rate of waves is maximal when the angle θ between the direction of the interplanetary magnetic field and the front of the bow shock is not equal . The dependence of the increment of perturbation on the solar wind velocity is analysed. A satisfactory agreement between theory and experimental results on the connection of Pc3–4 properties and parameters of the solar wind is obtained. 相似文献
15.
One of the goals of comet research is the determination of the chemical composition of the nucleus because it provides us
with the clues about the composition of the nebula in which comet nuclei formed.
It is well accepted that photo-chemical reactions must be considered to establish the abundances of mother molecules in the
coma as they are released from the comet nucleus or from distributed dust sources in the coma. However, the mixing ratios
of mother molecules in the coma changes with heliocentric distance. To obtain the abundances in the nucleus relative to those
in the coma, we must turn our attention to the release rates of mother molecules from the nucleus as a function of heliocentric
distance. For this purpose, we assume three sources for the coma gas: the surface of the nucleus (releasing mostly water vapor),
the dust in the coma (the distributed source of several species released from dust particles), and the interior of the porous
nucleus (the source of many species more volatile than water). The species diffusing from the interior of the nucleus are
released by heat transported into the interior. Thus, the ratio of volatiles relative to water in the coma is a function of
the heliocentric distance and provides important information about the chemical composition and structure of the nucleus.
Our goal is to determine the abundance ratios of various mother molecules relative to water from many remote-sensing observations
of the coma as a function of heliocentric distance. Comet Hale-Bopp is ideal for this purpose since it has been observed using
instruments in many different wavelength regions over large ranges of heliocentric distances. The ratios of release rates
of species into the coma are than modeled assuming various chemical compositions of the spinning nucleus as it moves from
large heliocentric distance through perihelion. Since the heat flow into the nucleus will be different after perihelion from
that before perihelion, we can also expect different gas release rates after perihelion compared to those observed before
perihelion. Since not all the data are available yet, we report on progress of these calculations.
This revised version was published online in July 2006 with corrections to the Cover Date. 相似文献
16.
We propose an interpretation of the enrichments in volatiles observed in the four giant planets with respect to the solar abundance. It is based on the assumption that volatiles were trapped in the form of solid clathrate hydrates and incorporated in planetesimals embedded in the feeding zones of each of the four giant planets. The mass of trapped volatiles is then held constant with time. The mass of hydrogen and of not trapped gaseous species continuously decreased with time until the formation of the planet was completed, resulting in an increase in the ratio of the mass of trapped volatiles to the mass of hydrogen (Gautier et al., Astrophys. J. 550 (2001) L227). The efficiency of the clathration depends upon the amount of ice available in the early feeding zone. The quasi-uniform enrichment in Ar, Kr, Xe, C, N, and S observed in Jupiter is reproduced because all volatiles were trapped. The non-uniform enrichment observed in C, N and S in Saturn is due to the fact that CH4, NH3, and H2S were trapped but not CO and N2. The non-uniform enrichment in C, N and S in Uranus and Neptune results from the trapping of CH4, CO, NH3 and H2S, while N2 was not trapped. Our scenario permits us to interpret the strongly oversolar sulfur abundance inferred by various modelers to be present in Saturn, Uranus and Neptune for reproducing the microwave spectra of the three planets. Abundances of Ar, Kr and Xe in these three are also predicted. Only Xe is expected to be substantially oversolar. The large enrichment in oxygen in Neptune with respect to the solar abundance, calculated by Lodders and Fegley (Icarus 112 (1994) 368) from the detection of CO in the upper troposphere of the planet, is consistent with the trapping of volatiles by clathration. The upper limit of CO in Uranus does not exclude that this process also occurred in Uranus. 相似文献
17.
18.
In this paper we examine the recently introduced Dvali-Gabadadze-Porrati (DGP) gravity model. We use a space-time metric in which the local gravitation source dominates the metric over the contributions from the cosmological flow. Anticipating ideal possible solar system effects, we derive expressions for the signal time delays in the vicinity of the Sun. and for various ranges of the angle θ of the signal approach, The time contribution due to DGP correction to the metric is found to be proportional to b 3/2/c 2 r 0. For r 0 equal to 5 Mpc and θ in the range [−π/3,π/3], Δt is equal to 0.0001233 ps. This delay is extremely small to be measured by today’s technology but it could be probably measurable by future experiments. 相似文献
19.
A. P. Markeev 《Astronomy Letters》2001,27(7):475-479
The centers of the gaps observed in the asteroid belt are displaced toward Jupiter from their positions that correspond to the exact commensurability between the mean motions of an asteroid and Jupiter. Using the current theory of stability and nonlinear oscillations of Hamiltonian systems, we point out the dynamical causes of this asymmetry. Our analysis is performed in terms of the plane circular restricted three-body problem. The orbits that correspond to Poincaré periodic solutions of the first kind are taken as unperturbed asteroid orbits. 相似文献
20.
X-ray photographs obtained with a zone plate camera on October 3, 1967 in the wavelength band 49.5–52.5 Å have been investigated photometrically.The most intense X-ray emission corresponds with active regions in H and Ca ii. About one quarter of the total solar flux is emitted by the three brightest X-ray sources (A, E and J). X-ray emission from quiet regions is also observed. Limb brightening is found, also at the poles, which indicates a higher electron density at the poles than during solar minimum.The brightest X-ray regions have a very small core of the order of 20. No relation to magnetic field strengths of sunspots has been found. However, a correlation with active prominences cannot be ruled out. X-ray source A is related either to prominence activity or to flare activity. One X-ray region (J) is probably related to flare activity.Assuming an electron temperature of 3 × 106K to 5 × 106K for coronal active regions an emission measure of a few times 1049 cm–3 is derived, which yields an electron density of a few times 1010 cm–3. 相似文献