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1.
李小聪  Wegner  R 《天体物理学报》1995,15(4):313-322
本文讨论BLO0716+714中观测到的光学和射电快速变化(IDV)的相关性及可能的解释。详细的分析表明,这种相关性有三个特点:(1)光学变化和5GHz射电变化呈反相关,即光学极大和5GHz射电极小相对应,反之亦然;(2)光学变化和射电频谱指数α5^8.3的变化相关,具体地说,光学的增强和极大都与射电频谱反转频率向高频的位移有关;(3)光学和射电都有 ̄1天的准周期变化,特别是射电频谱指数α5^8.  相似文献   

2.
用美国甚大阵(VLA)对色球活动性双星系统UXAri进行了从1.4GHz到15GHz范围内五个频段的观测,观测期间UXAri处于活动性比较低的阶段,射电光度为(6.6-12.6)×1016ergs-1Hz-1.射电频谱低频部分比较平坦,高频呈幂律形式,低频的圆偏振度很低,趋于零,高频辐射有中等圆偏振度(15%).射电发射机制可能是回旋同步加速机制,由此我们估计出发射区的磁场强度为几至几十高斯,相对论电子密度为~104-102cm-3量级,热电子数密度~108cm-3。  相似文献   

3.
一个新型分米波太阳微耀斑现象的观测分析   总被引:1,自引:0,他引:1  
本介绍一组短分米波(1.42GHz)太阳微耀斑的射电和光学辐射特征,它们包含3个叠加在连续辐射背景上的射电快速精细结构(FFS),即准周期快速脉冲链(称微耀斑)它们的形态相似,强度大约在150-200sfu范围内,其寿命(半功率宽)大多为15-50ms,有18个分离的双峰结构,该事件产生的7646活动区中出现两处新浮现的几个小黑子,呈现复杂极性,可能存在多重交叉小磁流环多次重联的复杂状况,本定  相似文献   

4.
为了解释Blazar天体射电爆发的普遍演化特性,本提出一个持续注入的喷流模型。假定在喷流基底上以相对论性速度持续地注入相对论等离子体(由磁场和相对论电子组成)。这一等离子体在沿喷流向外运动时经受绝热膨胀损耗。理论计算表明,射电爆发的频谱演化具有Valtaoja等人所建议的典型的3阶段演化形式。它们非常好地重现了Blazar天体中观测到的射电爆发的普遍行为。  相似文献   

5.
南天区20个河外射电源的VLBI研究   总被引:6,自引:5,他引:1  
本报道南天区5GHz普查式观测结果,首次观测是在1992年11月期间进行的,共观测23个河外射电源,获得了20个河外射电源的VLBI高分辨率的射电图象,有15个射电源呈现核喷流结构,1个有双向喷流,3个未分解,未发现有致密双源,在16个核喷流(包括一个双向喷流源)源中有11个呈现弯曲喷流现象。此外还首次发现了3个源中可能有超光速运动现象。  相似文献   

6.
1993年5月30日22GHz的缓变型射电事件的时间轮廓特征,以及在3GHz,10GHz频率上没有对应射电事件的观测特征等,可用Matzler的热模型得到合理的解释。  相似文献   

7.
1993年5月30日22GHz的缓变型射电事件的时间轮廓特征,以及在3GHz、10GHz频率上没有对应射电事件的观测特征等,可用Matzler的热模型得到合理的解释。  相似文献   

8.
在1991—1993年期间,Comptonγ射线天文台(CGRO)在射电源PKS0528+134中观测到两次很强的射线爆发,都伴随有毫米波射电大爆发.本文详细分析了高能γ-X射线波段和红外-光学波段的辐射能量分布(SED).结果表明,高能γ射线辐射可能主要是由喷流相对论电子对周围UV-软X射线光子的逆康普顿散射所产生的.同时,通过毫米波射电大爆发的频谱演化特性与γ射线源的同步辐射频谱特性的比较,对γ辐射等离子团和射电等离子团之间可能的演化联系作了讨论.  相似文献   

9.
正在发展中的云南天文中0.5GHz-1.5GHz快速射电频谱分析仪的接收天线部分是计划在现有十米口径抛物面天线的焦点上安装两付互相垂直的对数周期偶极子天线作为馈源。本文介绍了设计一个FORTRAN语言程序对对数周期偶极子天线电特性进行分析的过程它可以在整个工作频段范围内计算出任意频率点上一副和周期偶极子天线两个主平面内的方向图、波瓣宽度、增益和输入阻抗,并把结果以数据文件的形式记录下来,结合  相似文献   

10.
云南天文台“四波段(1.42GHz,2.13GHz,2.84GHz和4.26GHz)太阳射电高时间同步观测系统”在1990.1 ̄1994.1期间,观测到5个具有短时标漂移结构的射电爆发事件,也就是微波Ⅲ型爆发。本文从中选取较典型的1991年3月13日事件,对Ⅲ型爆发的时间轮廓(持续时间,衰减时间)作了分析,并与米波,分米波和微波段其它观测结果作了一些比较,以求对长厘米 ̄短分米波段(微波低端)Ⅲ型爆  相似文献   

11.
Observational data on the dynamics of stars in the neighborhood of the sun indicate the existence of a third integral besides the integrals of the angular momentum and energy. The Poincaré integral is proposed as a third integral. The consequences of this assumption are derived and compared with available astrophysical data.  相似文献   

12.
介绍和论述了在后牛顿引力理论(PPN形式)中在优越参考系和非优越参考系中经过参数化后引力常数变化对地球自转产生的效应,其中特别重点介绍了年周期变化的效应。此外也将理论结果同观测结果相对比。  相似文献   

13.
耀变体(Blazars)的亮温度与黑洞喷流能量和吸积率有重要关系.搜集了53个耀变体源样本,包括22个蝎虎天体(BL Lacs)和31个平谱射电类星体(Flat Spectrum Radio Quasars,FSRQs),研究了耀变体亮温度与黑洞喷流能量的分布,并对子类中亮温度与黑洞喷流能量的相关性进行了讨论.研究结果...  相似文献   

14.
We have developed a cosmological model for the Earth rotation and planetary acceleration that gives a good account (data) of the Earth astronomical parameters. These data can be compared with the ones obtained using space-base telescopes. The expansion of the universe has shown to have an impact on the rotation of planets, and in particular, the Earth. The expansion of the universe causes an acceleration that is exhibited by all planets.  相似文献   

15.
We present the design concept of the spectropolarimeter for the high‐resolution echelle spectrograph PEPSI tobe installed at the 2 × 8.4 m Large Binocular Telescope (LBT) in Arizona. We discuss the optical key elements, the principles of operations of the instrument and its instrumental polarization effects (© 2011 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)  相似文献   

16.
Range of values of the Sun's mass quadrupole moment of coefficient J2 arising both from experimental and theoretical determinations enlarge across literature on two orders of magnitude, from around 10-7 until to 10-5. The accurate knowledge of the Moon's physical librations, for which the Lunar Laser Ranging data reach an outstanding precision level, prove to be appropriate to reduce the interval of J2 values by giving an upper bound of J2. A solar quadrupole moment as high as 1.1 10-5 given either from the upper bounds of the error bars of the observations, or from the Roche's theory, is not compatible with the knowledge of the lunar librations accurately modeled and observed with the LLR experiment. The suitable values of J2 have to be smaller than 3.0 10-6. As a consequence, this upper bound of 3.0 10-6 is accepted to study the impact of the Sun's quadrupole moment of mass on the dynamics of the Earth-Moon system. Such as effect (with J2 = 5.5±1.3 × 10-6) has been already tested in 1983 by Campbell & Moffat using analytical approximate equations, and thus for the orbits of Mercury, Venus, the Earth and Icarus. The approximate equations are no longer sufficient compared with present observational data and exact equations are required. As if to compute the effect on the lunar librations, we have used our BJV relativistic model of solar system integration including the spin-orbit coupled motion of the Moon. The model is solved by numerical integration. The BJV model stems from general relativity by using the DSX formalism for purposes of celestial mechanics when it is about to deal with a system of n extended, weakly self-gravitating, rotating and deformable bodies in mutual interactions. The resulting effects on the orbital elements of the Earth have been computed and plotted over 160 and 1600 years. The impact of the quadrupole moment of the Sun on the Earth's orbital motion is mainly characterized by variations of , , and . As a consequence, the Sun's quadrupole moment of mass could play a sensible role over long time periods of integration of solar system models. This revised version was published online in July 2006 with corrections to the Cover Date.  相似文献   

17.
By means of a simple relation between the velocity v of the fluid particle and the velocity vf of the photospheric footpoint of the magnetic field line vz and Bz being respectively the components of v and the magnetic field B normal to the photospheric surface, it is shown formally that through the phtospheric surface the transport of all the quantities attributed to the magnetic field, such as the magnetic flux, the magnetic energy and the helicity, is independent of vz, and vf is the only kinematical quantity on which the transport depends. In addition, in the neighborhood of the neutral line the velocity vl of the moving curve of constant Bz is found to be equal approximately to the component of v or vf in the direction of vl. Since vl can be measured or extimated, so can the components of v and vf near the neutral line.  相似文献   

18.
The solar system's position in the Galaxy is an exclusive one, since the Sun is close to the corotation circle, which is the place where the angular velocity of the galactic differential rotation is equal to that of density waves displaying as spiral arms. Each galaxy contains only one corotation circle; therefore, it is an exceptional place. In the Galaxy, the deviation of the Sun from the corotation is very small — it is equal to ΔR/R ≈0.03, where ΔR=R c ?R ,R c is the corotation distance from the galactic center andR is the Sun's distance from the galactic center. The special conditions of the Sun's position in the Galaxy explain the origin of the fundamental cosmogony timescalesT 1≈4.6×109 yr,T 2?108 yr,T 3?106 yr detected by the radioactive decay of various nuclides. The timescaleT 1 (the solar system's ‘lifetime’) is the protosolar cloud lifetime in a space between the galactic spiral arms. The timescaleT 2 is the presolar cloud lifetime in a spiral arm.T 3 is a timescale of hydrodynamical processes of a cloud-wave interaction. The possibility of the natural explanation of the cosmogony timescales by the unified process (on condition that the Sun is near the state of corotation) can become an argument in favour of the fact that the nearness to the corotation is necessary for the formation of systems similar to the Solar system. If the special position of the Sun is not incidental, then the corotation circles of our Galaxy, as well as those of other galaxies, are just regions where situations similar to ours are likely to be found.  相似文献   

19.
Perturbations in the motion of the Moon are computed for the effect by the oblateness of the Earth and for the indirect effect of planets. Based on Delaunay's analytical solution of the main problem, the computations are performed by a method of Fourier series operation. The effect of the oblateness of the Earth is obtained to the second order, partly adopting an analytical evaluation. Both in longitude and latitude are found a few terms whose coefficient differs from the current lunar ephemeris based on Brown's theory by about 0.01. While, concerning the indirect effect of planets, several periodic terms in the current ephemeris seem to have errors reaching 0.05.As for the secular variations of and due to the figure of the Earth and the indirect effect of planets, the newly-computed values agree within 1/cy with Brown's results reduced to the same values of the parameters. Further, the accelerations in the mean longitude, and caused by the secular changes in the eccentricity of the Earth's orbite and in the obliquity of the ecliptic are obtained. The comparison with Brown shows an agreement within 0.3/cy2 for the former cause and 0.02/cy2 for the latter. An error is found in the argument of the principal term for the perturbations due to the ecliptic motion in the current ephemeris.Proceedings of the Conference on Analytical Methods and Ephemerides: Theory and Observations of the Moon and Planets. Facultés universitaires Notre Dame de la Paix, Namur, Belgium, 28–31 July, 1980.  相似文献   

20.
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