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1.
研究表明,高频射电源与低频射电源相比,前者中的类星体比例更大。3CR低频射电源(S178MHz>9Jy)中有17.8%是类星体,而在2.7GHz亮射电源样本中(S2.7GHz≥2.0Jy),有35.6%是类星体。更有趣的是,518个5GHz亮射电源中(S5GHz≥1.0Jy),至少有291个(≥56%)是类星体。因此,我们认为高频亮射电源的证认是发现类星体的有效手段。  相似文献   

2.
光学观测表明,致密星系群SCGG 223中成员星系的速度弥散高达1106km/s,并且 整个星系群处于平衡状态.星系群的数值模拟也显示, SCGG 223是维里化的.这些光学 波段上的研究结果暗示, SCGG 223可能具有星系团量级的大引力质量,其星系际气体则 很可能处在极高温的状态.为了证实这些推测,作者在 1999年 2月利用 ASCA卫星对 SCGG 223进行了 X射线观测.通过光谱分析,获得了它的气体温度和 0.5~10 keV波段 上的光度分别为kT=1.4_(-0.4)~(+.6): keV和9.85_(-2.04)~(6.11)× 1036J S-1.与光学观测所作出的预计相 反,这些数值显示 SCGG 223是一个正常的低温星系群.由于 SCGG 223在 0.5~10 keV 波段上很暗,无法从ASCA获得的X射线表面亮度分布推算其总引力质量,因此,尚不 能直接判断它的质量是否真的像光学维里质量那样大.  相似文献   

3.
从ROSAT PSPC观测数据中我国发现了与PSR0355+54相关联的脉冲星X射线喷流存在的证据。这是一个与脉冲星自行方向相反的长度为12′的近似线性的辐射特征。假设喷流具有PSR0355+54相同的距离和星际吸收,而其能谱是谱指数为-0.5的幂律谱,可导出喷流的光度为2.48±0.83×10^24J/S。喷流中的平均磁场约为7.9×10^-9T,典型的电子能量为2.1×10^7MeV。  相似文献   

4.
利用紫金山天文台青海观测站13.7米射电望远镜对源IRAS053910217和IRAS065720742进行了12COJ=1-0观测,获得了气体的相应参数;用IRAS及其他红外观测资料,获得了尘埃热结构;探讨了云中气体的热平衡.对于IRAS053910217中由远红外得出的Td<Tk的情形,考虑了几种可能的加热机制.光电加热对该云可能是比较重要的;激波可能是另一种加热途径.  相似文献   

5.
1995年5月,使用2.16m望远镜对ROSAT X射线源进行光学证认期间,发现8个ROSAT X射线源和5G射电源的光学对应体是以前未发现的类星体,其红移范围从0.333至1.091。本文给出了这些类星体的多波段特性。  相似文献   

6.
利用紫金山天台青海站的13.7m毫米波望远镜,对OrionA分子云中的OMC-3区域,进行了较高分辨率的^13CO(J=1-0)和C^18O(J=1-0)分子辐射的图观测,给出了该分子云中^13CO和C^18O的云核中心分别与最年龄的天体-Class0类源MMSI,MMS4,MMS6和MMS7,MMS8,MMS9成协,此外,通过分析OMC-3整个区域的速度场结构,发现沿C^18O和^13CO云核  相似文献   

7.
利用紫金山天文台青海站的 13.7 m毫米波望远镜,对 Orion A分子云中的 OMC-3区域,进行了较高分辨率的13CO(J=1-0)和C18O(J=1-0)分子辐射的成图观测.给出了该分子云中13CO和 C18O云核分布的整体结构和平均物理参数.观测发现,该分子云的13CO和 C18O的云核中心分别与最年轻的天体-Class 0类源 MMSI, MMS4,MMS6和MMS7,MMS8;MMS9成协.此外,通过分析OMC-3整个区域的速度场结构,发现沿 C18O和13CO云核方向从南到北有一个~ 1.7km/s的速度场梯度,而分子云的红、蓝移团块则分别趋于云的北部和南部.并对OMC-3区的恒星形成特征进行了讨论.  相似文献   

8.
脉冲星PSR B0329+54的多波段观测   总被引:2,自引:0,他引:2  
给出1999年3月12日至6月8日,使用国家天文观测中心乌鲁木齐南山站25m射电望远镜在0.327GHz,1.5GHz,2.3GHz,4.8GHz和8.4GHz频段,对脉冲星PSRB0329+54进行的多波段观测结果,PSRB0329+54的辐射呈幂律谱,并出现频谱转折现象,低频段谱指数为1.59,高频段为2.45,平均谱指数为1.72五个频段上的平均脉冲轮廓的角宽度和二个民分峰值间的角宽度都随频  相似文献   

9.
1995年5月,使用2.16m望远镜对ROSATX射线源进行光学证认期间,发现8个ROSATX射线源和5G射电源的光学对应体是以前未发现的类星体,其红移范围从0.333至1.091。本文给出了这些类星体的多波段特性。  相似文献   

10.
用紫金山天文台青海站的137m射电望远镜,对10个行星状星云给出了新的CO(1-0)谱线观测结果.其中4个行星状星云:NGC6445,M159,M49和M251,已有过CO(21)的观测,本文第一次给出了它们的CO(10)的测量结果;对2个别人曾经观测过但未测到CO的行星状星云:Sh271和M418,本文第一次证认了它们的CO发射;对4个别人从未进行过CO搜寻的行星状星云:VV18,M252,He2459和K331,本文第一次进行了观测,并得到了它们的CO(10)谱.由CO的发射谱征可见,VV18可能是一个误分类的行星状星云  相似文献   

11.
Non-thermal X-rays and very high energy (VHE) γ-rays have been detected from the supernova remnant (SNR) RX J1713.7−3946, and the recent observations with the Suzaku satellite clearly reveal a spectral cut-off in the X-ray spectrum, which directly relates to the cut-off of the energy spectrum of the parent electrons. However, whether the origin of the VHE γ-rays from the SNR is hadronic or leptonic is still in debate. We studied the multi-band non-thermal emission from RX J1713.7−3946 based on a semi-analytical approach towards the non-linear shock acceleration process by including the contribution of the accelerated electrons to the non-thermal radiation. The results show that the multi-band observations on RX J1713.7−3946 can be well explained in the model with appropriate parameters, and the TeV γ-rays have hadronic origin, i.e. they are produced via proton–proton interactions as the relativistic protons accelerated by the shock collide with the ambient matter.  相似文献   

12.
In this paper we show how to calculate the neutrino flux from a resolved source of high energy gamma-rays, of which have been measured fluxes and spectral indexes of each of the parts in which has been divided for the observations. For the calculation of the neutrino flux need to know the theoretical photon/neutrino ratios and have to consider the oscillation probability of neutrinos. As a numerical example the case of the Supernova Remnant RX J1713.7-3946 observed by H.E.S.S. experiment is presented here. Gamma-rays up to tens of TeV have been observed from RX J1713.7-3946, making this source a possible site of hadronic interactions and thus a source of neutrinos. The H.E.S.S. experiment observed 14 different regions in RX J1713.7-3946, measuring in each one the gamma-ray flux and spectral index. The technique presented in this paper can be applied to other high energy astrophysical sources, point-like or resolved.  相似文献   

13.
We investigate a possibility that non-thermal X-ray emission in a supernova remnant(SNR) is produced by jitter radiation, which is the analogue of synchrotron radiation in small-scale random magnetic fields. We can fit the multi-wavelength data of SNRs RX J1713.7-3946 (G347.3-0.5) and RX J0852.0-4622 (G266.6-1.2) by constructing pure jitter and inverse Compton (IC) emission models. We find that the physical fit parameters of random magnetic fields take values of several tens of μG strength and of the order of ∼107 cm correlation length. These properties of random magnetic fields in collisionless shock of SNRs are discussed.   相似文献   

14.
We study the individual contribution to secondary lepton production in hadronic interactions of cosmic rays (CRs) including resonances and heavier secondaries. For this purpose we use the same methodology discussed earlier [C.-Y. Huang, S.-E. Park, M. Pohl, C.D. Daniels, Astropart. Phys. 27 (2007) 429], namely the Monte-Carlo particle collision code DPMJET3.04 to determine the multiplicity spectra of various secondary particles with leptons as the final decay states, that result from inelastic collisions of cosmic-ray protons and Helium nuclei with the interstellar medium of standard composition. By combining the simulation results with parametric models for secondary particle (with resonances included) for incident cosmic-ray energies below a few GeV, where DPMJET appears unreliable, we thus derive production matrices for all stable secondary particles in cosmic-ray interactions with energies up to about 10 PeV.

We apply the production matrices to calculate the radio synchrotron radiation of secondary electrons in a young shell-type SNR, RX J1713.7-3946, which is a measure of the age, the spectral index of hadronic cosmic rays, and most importantly the magnetic field strength. We find that the multi-mG fields recently invoked to explain the X-ray flux variations are unlikely to extend over a large fraction of the radio-emitting region, otherwise the spectrum of hadronic cosmic rays in the energy window 0.1–100 GeV must be unusually hard.

We also use the production matrices to calculate the muon event rate in an IceCube-like detector that are induced by muon neutrinos from high-energy γ-ray sources such as RX J1713.7-3946, Vela Jr. and MGRO J2019+37. At muon energies of a few TeV, or in other word, about 10 TeV neutrino energy, an accumulation of data over about 5–10 years would allow testing the hadronic origin of TeV γ-rays.  相似文献   


15.
The Fermi γ-ray space telescope reported the observation of several Galactic supernova remnants recently, with the γ-ray spectra well described by hadronic pp collisions. The possible neutrino emissions from these Fermi detected supernova remnants are discussed in this work, assuming the hadronic origin of the γ-ray emission. The muon event rates induced by the neutrinos from these supernova remnants on typical km3 neutrino telescopes, such as the IceCube and the KM3NeT, are calculated. The results show that for most of these supernova remnants the neutrino signals are too weak to be detected by the on-going or up-coming neutrino experiment. Only for the TeV bright sources RX J1713.7-3946 and possibly W28 the neutrino signals can be comparable with the atmospheric background in the TeV region, if the protons can be accelerated to very high energies. The northern hemisphere based neutrino telescope might detect the neutrinos from these two sources.  相似文献   

16.
In 2004 and 2005, the shell-type supernova remnants RX J1713.7–3946 and RX J0852.0–4622 were observed and detected with the complete H.E.S.S. array, a system of four Imaging Cherenkov Telescopes located in Namibia and dedicated to the observations of γ-rays above 100 GeV. The energy spectra of these two sources have been measured over a wide energy range and revealed an integral flux above 1 TeV similar to that of the Crab Nebula. Their morphologies were resolved with high accuracy with H.E.S.S. and exhibit a striking correlation with the X-ray images, thereby pioneering a technique of unambiguously identifying spatially extended γ-ray sources. The results of the observations will be presented. Similarities and differences between these two sources will be pointed out as well as possible implications. M. Lemoine-Goumard, F. Aharonian, D. Berge, B. Degrange, D. Hauser, N. Komin, O. Reimer, U. Schwanke for the H.E.S.S. Collaboration  相似文献   

17.
Stimulated by the recent discovery of PSR J1833-1034 in SNR G21.5-0.9 and its age parameters presented by two groups of discovery, we demonstrate that the PSR J1833-1034 was born 2053 years ago from a supernova explosion, the BC 48 guest star observed in the Western Han (Early Han) Dynasty by ancient Chinese. Based on a detailed analysis of the Chinese ancient record of the BC 48 guest star and the new detected physical parameters of PSR J1833-1034, agreements on the visual position, age and distance between PSR J1833-1034 and the BC 48 guest star are obtained. The initial period P0 of PSR J1833-1034 is now derived from its historical and current observed data without any other extra assumption on P0 itself, except that the factor PP is a constant in its evolution until now.  相似文献   

18.
Spectroscopic and infrared observations of Comet Sugano-Saigusa-Fujikawa (1983V) were obtained during its close approach to the Earth on 11-14 June 1983. The [O I] production rates of 1.8 +/- 0.9 x 10(26) atoms/s observed on 12.3 June and 7 +/- 3.5 x 10(26) atoms/s on 13.4 June lead to derived water-production rates of 3 x 10(27) mol/s on 12 June and 1.1 x 10(28) mol/s on 13 June. The abundances of the minor species NH2, CN, C2, and C3 are unusually low relative to [O I]. The upper limit to the average nuclear radius from our infrared and visual photometry on 12-13 June (assuming that the entire signal came from the nucleus) is approximately 370 m. The dust/gas mass ratio was <0.01 on June 12 and <0.005 on June 13.  相似文献   

19.
We describe measurements of the mirror vignetting in the XMM-Newton Observatory made in-orbit, using observations of SNR G21.5-09 and SNR 3C58 with the EPIC imaging cameras. The instrument features that complicate these measurements are briefly described. We show the spatial and energy dependences of measured vignetting, outlining assumptions made in deriving the eventual agreement between simulation and measurement. Alternate methods to confirm these are described, including an assessment of source elongation with off-axis angle, the surface brightness distribution of the diffuse X-ray background, and the consistency of Coma cluster emission at different position angles. A synthesis of these measurements leads to a change in the XMM calibration data base, for the optical axis of two of the three telescopes, by in excess of 1 arcmin. This has a small but measureable effect on the assumed spectral responses of the cameras for on-axis targets. This revised version was published online in July 2006 with corrections to the Cover Date.  相似文献   

20.
We present the results of magnetic field measurements in three active prominences, July 24, 1981, July 24, 1999, and July 12, 2004, obtained from observations with the echelle spectrograph of the horizontal solar telescope at the Astronomical Observatory of the Taras Shevchenko Kiev National University. The magnetic fields were measured from the Zeeman splitting of the I ± V profiles in the He I D3 and H?? lines in the atmosphere at heights from 3 to 14 Mm. Our measurements of the effective magnetic fields B eff from the shift of the profile centroids have shown that the magnetic fields averaged over the entrance slit area were within the range from ?600 to +1500 G. The amplitude values of the local fields have been estimated from the splitting of the bisectors of the central parts of the line profiles at 0.9 of the peak intensity. The corresponding fields B 0.9 have turned out to be approximately twice B eff and reached 4000 G in absolute value. Narrow (1?C2 Mm) height peaks at heights of 6?C11 Mm have been found in the height distributions of the magnetic field. We have found an interesting effect in two prominences-an anticorrelation between the magnetic field strengths measured from the D3 and H?? lines.  相似文献   

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