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1.
用澳大利亚悉尼大学的Fleurs综合孔径射电望远镜,在1415MHz上对两个南天射电星系PKS1331-09和PKS1417-20进行了观测,得到了分辨率约为40弧秒的射电亮度分布图,并求得了它们的几何参数和物理参数.前者是一个延伸达1.9 Mpc的巨射电星系,具有与CygA十分相似的双源结构.我们猜测用更高分辨率观测该源时,可期望在它的子源外边沿发现热斑结构;后者是一通常的晕核结构源.  相似文献   

2.
用4km Ooty综合孔径射电望远镜,来研究Abell星系团A514在326.5MHz上的射电结构。该文给出了A514星系团中四个射电星系(射电源)的射电图,并作了初步分析,得出射电星系的某些结构特性及其物理参数。  相似文献   

3.
本文介绍了高红移射电星系近年来的研究进展。新的天文观测手段和技术方法的发展,导致了一批高红移射电星系的发现。多波段的联合研究,揭示了出高红移射电星系光学/红外辐射与射电结构之间的成协现象。开发这些亮而远的射电星系研究有助于我们了解早期的演2化及星系活动的内在原因。  相似文献   

4.
本文叙述用荷兰威斯特堡3公里基线射电望远镜对射电星系3C390.3进行的0.6京赫射电观测。3C390.3是一个边缘增亮型双子源射电源,在热斑与中心核源之间有强的桥状结构把二者连接起来。观测到复杂的线偏振结构:南部子源有双重结构,北部子源有三重结构。本文还把新观测与1.5公里基线1.4京赫的观测进行了比较,从而导出了源区一些重要的物理参数。  相似文献   

5.
从射电结构的角度评述了BLLac天体和FR-I射电星系的统一模型的最新进展,内容包括射电结构、延展射电光度(Pext)、最大角尺度(LAS)、射电核主导系数(f)的比较以及对相对论聚束的测试。最新的射电观测资料表明XBLs是介于FR-I和RBLs之间的过渡型天体,这为BLLac天体是聚束的FR-I射电星系提供了一个很好的证据。  相似文献   

6.
射电星系根据射电形态可以分为FRⅠ和FRⅡ两类,而根据其光学光谱特征可以分为低激发和高激发射电星系。它们在观测上表现出不同,其原因并不清楚,部分原因是喷流与周围介质的相互作用导致的,也可能是因为FR Ⅰ和FR Ⅱ的中央引擎吸积模式不同导致的。为了检验这些源是否存在尘埃环,用CLOUDY程序模拟3C 288射电源的光致电离模型,发现理论得到的电离光度远大于实际观测到的光学核光度,这说明在3C 288中确实存在遮挡效应。为了进一步检验这个结论,又根据尘埃消光来验证高喷流射电功率星系中的遮挡效应是尘埃环造成的。  相似文献   

7.
从射电结构的角度评述了BLLac天体和FR-I射电星系的统一模型的最新进展,内容包括射电结构,延展射电光度(Pext),最大角尺度(LAS),射电核主导系数(f)的比较以及对相对论聚束的测试。最新的射电观测资料表明XBLs是介于FR-I和RBLs之间的过渡型天体,这对BLLac天体是聚束的FR-I射电星系提供了一个很好的证据。  相似文献   

8.
利用30颗左右射电星的光学和射电位置,在坐标和自行系统、参考星表及位置历元统一的基础上,得到了光学系统与射电系统间的转动参数的初步结果。  相似文献   

9.
基于被ROSAT全天区巡天观测和射电 4.85GHz巡天观测同时探测到的活动星系核的大样本 ,研究了X射线选的射电噪活动星系核的多波段性质 .通过分析该样本中的活动星系核的宽波段能量分布 ,确认了来自射电、光学和X射线波段的辐射光度之间的显著相关性 .这种相关性对于类星体、赛弗特、蝎虎座天体和射电星系是有区别的 .同时 ,探讨了从光学到X射线波段之间的谱指数与红移以及 50 0 0 和 4.85GHz处的单色光度的相关性  相似文献   

10.
云南天文台高分辨率射电频谱仪观测到10毫秒级变周期振荡,带宽约10MHz,叠加在一个持续时间约500ms的射电频谱上.在德国Weissenau的太阳射电频谱记录上找到了对应的爆发;同时SESC(美国空间环境服务中心)发表了同一时刻获得的245MHz总强度射电爆发记录;还在日面城到了相应的H_α亮点.  相似文献   

11.
1991年3月,我们利用上海25m射电望远镜和欧洲VLBI网联合对几个河外射电源进行了第二历元的327MHzVLBI观测.数据的相关处理先后在上海天文台三台站MK2相关处理机和美国的Caltech/JPL相关处理机进行,以便于比较相关结果。本文给出3C84、3C345和3C380的混合图。与第一历元的观测比较,3C345和3C380的流量密度没有明显的变化,但3C345的结构变化明显。3C84和3C345有喷流的迹象.3C454.3的总流量在不到两年的时间内增加了25%,如果这个变化是内禀的话,那么可能意味着一次新的流量爆发。  相似文献   

12.
Most of the radio galaxies with z > 3 have been found using the red-shift spectral index correlation. We have started a programme with the Giant Metrewave Radio Telescope (GMRT) to exploit this correlation at flux density levels about 100 times deeper than the known high-redshift radio galaxies, with an aim to detect candidate high-redshift radio galaxies. Here we present results from the deep 150 MHz observations of LBDS-Lynx field, which has been imaged at 327, 610 and 1412 MHz with the Westerbork Synthesis Radio Telescope (WSRT) and at 1400 and 4860 MHz with the Very Large Array (VLA). We find about 150 radio sources with spectra steeper than 1. About two-thirds of these are not detected in Sloan Digital Sky Survey (SDSS), hence are strong candidate high-redshift radio galaxies, which need to be further explored with deep infra-red imaging and spectroscopy to estimate the red-shift.  相似文献   

13.
Seven giant radio pulses were recorded from the millisecond pulsar PSR B1937+21 during ≈8.1 min observation by the Ooty Radio Telescope (ORT) at 326.5 MHz. Although sparse, these observations support most of the giant pulse behaviour reported at higher radio frequencies (430 to 2380 MHz). Within the main component of the integrated profile, they are emitted only in a narrow (≲47 μs) window of pulse phase, close to its peak. This has important implications for doing super-high precision timing of PSR B1937+21 at low radio frequencies.  相似文献   

14.
The refraction of radio waves as they traverse through the terrestrial ionosphere and troposphere introduces a differential phase path which results for a radio interferometer in variations of the visibility phase. Though refraction due to troposphere is significant for synthesis radio telescopes operating at 1.0 GHz and above, ionospheric refraction is dominant at lower frequencies. This problem is important in the case of Ooty Synthesis Radio Telescope (OSRT) operating at 326.5 MHz, due to its proximity to the magnetic equator. This paper deals with the nature of phase variations suffered by OSRT due to refraction and explains the methodology evolved to alleviate them.  相似文献   

15.
Observations of the redshifted 21-cm HI fluctuations promise to be an important probe of the post-reionization era (z≤ 6). In this paper we calculate the expected signal and foregrounds for the upgraded Ooty Radio Telescope (ORT) which operates at frequency ν o = 326.5 MHz which corresponds to redshift z = 3.35. Assuming that the visibilities contain only the HI signal and system noise, we show that a 3 σ detection of the HI signal (~1 mK) is possible at angular scales 11 to 3° with ≈1000 h of observation. Foreground removal is one of the major challenges for a statistical detection of the redshifted 21 cm HI signal. We assess the contribution of different foregrounds and find that the 326.5 MHz sky is dominated by the extragalactic point sources at the angular scales of our interest. The expected total foregrounds are 104?105 times higher than the HI signal.  相似文献   

16.
We report the first measurements of radio frequency spectrum occupancy performed at sites aimed to host the future radio astronomy observatory in Indonesia. The survey is intended to obtain the radio frequency interference (RFI) environment in a spectral range from low frequency 10 MHz up to 8 GHz. The measurements permit the identification of the spectral occupancy over those selected sites in reference to the allocated radio spectrum in Indonesia. The sites are in close proximity to Australia, the future host of Square Kilometre Array (SKA) at low frequency. Therefore, the survey was deliberately made to approximately adhere the SKA protocol for RFI measurements, but with lower sensitivity. The RFI environment at Bosscha Observatory in Lembang was also measured for comparison. Within the sensitivity limit of the measurement equipment, it is found that a location called Fatumonas in the surrounding of Mount Timau in West Timor has very low level of RFI, with a total spectrum occupancy in this measured frequency range being about 1 %, mostly found at low frequency below 20 MHz. More detailed measurements as well as a strategy for a radio quiet zone must be implemented in the near future.  相似文献   

17.
The results of flux pulsar radioemission measurements at meter wavelengths, made at Pushchino Radio Astronomical Observatory of the Lebedev Physical Institute, are presented. Flux densities at 102, 85, 61 and 39 MHz have been measured for 85, 29, 37 and 23 pulsars correspondingly. Some of them were performed at all frequencies simultaneously. On the basis of these data and high frequencies data obtained by other authors, spectra of 52 pulsars were plotted. In practically all investigated pulsars we have detected a turn-over frequency at which the flux density of pulsar radioemission attained its maximum. Its mean value isv m =130±80 MHz. Averaged on many pulsars, the spectral index is negative in the 39–61 MHz frequency range and passes through zero at frequencies of about 100 MHz, becoming positive in the 100–400 MHz frequency range. It was noticed that the spectral index in the 100–400 MHz interval depends upon such pulsar periods as α100−=0.7logp+0.9. Using the spectra, more precise radio luminosities of pulsars have been computed.  相似文献   

18.
为了在云南天文台40 m天线上开展射电天文研究,使用它进行了河外射电源流量试观测。通过对河外致密源进行ON/OFF跟踪观测,得到射电源的流量变化曲线。但数据质量并不理想,说明系统存在一些问题。随后,根据对该望远镜系统的稳定性及其无线电环境干扰现状的考察,以及对现存问题的分析,提出了相应的解决方法。  相似文献   

19.
Cho  K.-S.  Kim  K.-S.  Moon  Y.-J.  Dryer  M. 《Solar physics》2003,212(1):151-163
A new solar radio spectrograph to observe solar radio bursts has been installed at the Ichon branch of the Radio Research Laboratory, Ministry of Information and Communication, Korea. The spectrograph consists of three different antennas to sweep a wide band of frequencies in the range of 30 MHz ∼ 2500 MHz. Its daily operation is fully automated and typical examples of solar radio bursts have been successfully observed. In this paper we describe briefly its hardware and data processing methods. Then we present coronal shock speeds estimated for 34 type II bursts from May 1998 to November 2000 and compare them with those from other observatories. We also present the close relationship between onset time of type II bursts and X-ray flares as well as their associations with coronal mass ejections.  相似文献   

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