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1.
通过对W3(OH)区域22GHzH2O脉泽源的短时间跟踪观测,探测到速度为-52 .8Km/s子谱的流量密度呈线性下降趋势,变化时村约为19天。同时也观测到了整个脉泽源的谱线宽度与该子谱的强度之间的相关变化。这些现象可能是由脉泽云之间的相互碰撞导致脉泽抽运率的变化所引起的。  相似文献   

2.
给出了1997年4月15日至17日在北京天台用2.16m望远镜卡焦光谱仪观测获得的6颗激变变星(AB Boo,UX UMa,T CrB,AH Her,Z Cam和V426 Oph)及3颗相关天体(UMa3,EG UMa和Leo3)的CCD光谱,并同时拍摄了5颗晚型星(3Dra,v Vir,ψLeo,34Boo和36Com)的CCD光谱,作为晚型星参考谱,测量了观测样本星的Hα和近红外CaⅡ的三重  相似文献   

3.
刘永翊 《天文学进展》1997,15(3):247-253
简要综述了近年来对于星际CH3OH脉泽的观测和研究成果,对CH3OH脉泽的性质从分类,生成区域及分布,辐射特性,运动状况等方面做了介绍,并阐明了理论上对其时变特性,激发机制及河外脉泽的探讨,最后对两种类型的CH3OH脉泽作了对比和讨论。  相似文献   

4.
本文给出利用中国、意大利、南非射电望远镜对一个近赤道源样本在5GHz频率上进行MK2VLBI普测中10颗弱源的相关流量和其中部分源用HartRAO望远镜观测的总流量值,作为进一步的MK3或VLBA记录系统的VLBI观测依据.  相似文献   

5.
用射电天文联合实验室紫金山天文台青海站13.7米望远镜,于1997年4月对97个水脉泽源做了CO(J=1-0)的巡测及部分成图观测,结果表明81个源的谱线适于作成协星体活动分析.经初步证认有外向流候选者33个,全部为首次给出高速范围.对其轮廓特点及与H2O脉泽辐射的关系作了简要讨论.CO高速气体和H2O脉泽的速度范围和峰值速度在多数情况下分别相符,这说明两者的激发可能相关.  相似文献   

6.
利用北京天文台具有CCD终端的60cm光学望远镜(V波段)观测射电源的光学对应体,得到了0716+714和0839+187精确的光学位置。参考星表采用拉帕尔玛(LaPalma)的18cm全自动子午环观测资料编制的CAMC星表,该星表是FK5星表系统。两颗源位置的内符精度约为0.″19,与其他作者给出的光学和射电位置观测结果分别进行了比较  相似文献   

7.
本文给出35个不同类型含SiO(v=1,J=1-0)脉泽发射的AGB星的近红外观测结果(其中包括6个Ⅰ型OH星,13个Ⅱ型OH星,9个仅有SiO脉泽的星以及7个无OH脉泽但有SiO和H2O脉泽的星).得出了它们的JHK星等和流量.同时经认证找出了它们对应的IRAS观测数据.通过对它们的近红外、中远红外以及OH射电资料的同时分析,得出了不同类型SiO脉泽星的色指数、谱斜率以及在近红外波段上拟合的等效黑体温度Teq.由红外及OH射电资料导出了其中心星的质量损失率M,并在此基础上结合已知的SiO脉泽源资料,找出了不同类型SiO脉泽星各量之间的关系.计算结果表明,SiO脉泽具有普遍性,在各类脉泽星中都可出现.SiO脉泽的光度与质量损失率弱相关,并且从(Mira)SiO到(OH/IR)SiO逐渐增加.SiO脉泽的流量与近红外“色”以及等效黑体温度Teq的关系较为密切.SiO脉泽积分流量的上限与IRAS在12μm和25μm上流量分别都相关.本文对SiO脉泽在AGB演化中的地位和特殊性进行了简单讨论.  相似文献   

8.
郑兴武 《天文学报》1996,37(4):387-395
利用甚长基线干涉仪,在1665MHz频率上,观测超致密氢II区G45.07+0.13的左右圆偏振羟基(OH)分子脉泽辐射.利用多条纹率成图方法,获得了这个区域20mas相对位置精度的脉泽结构图.除两个弱子源以外,所有脉泽子源都位于彗状结构氢II区“彗头”的前沿.脉泽团离致密氢II区中心投影距离为0".4.在完全饱和辐射的假设下,估计脉泽活动区具有氢分子数密度约为4.5×108(H2)cm-3.在脉泽源中,发现一对Zeeman对,从它们的LSR速度差,导出脉泽区的磁场约为3mG,方向为远离地球方向.在致密氢II区G45.07+0.13彗头附近的脉泽团的直径为6×1016cm.这与G34.03+0.2的观测结果很类似.这给解释彗状结构的氢II区的各种模型提供了一个可靠的观测约束条件.  相似文献   

9.
星际水脉泽源中高速气体的CO巡测   总被引:1,自引:1,他引:0  
用射电天联合实验紫金山天台青海站13.7米望远镜,于1997年4月对97个水脉泽源做了CO(J=1-0)的巡测及部分成图观测。结果表明81个源的谱线适于作成协星体活动分析。经初步认证认有外向流候选33个,全部为首次给出高速范围,对其轮廓特点及与H2O脉泽辐射的关系作了简要讨论,CO高速气体和H2O脉泽的速度范围和峰值速度在多数情况下的分别相符,这说明两的激发可能相关。  相似文献   

10.
通过对 W3(OH)区域 22 GHz H_(2)O脉泽源的短时间跟踪观测,探测到速度为-52.8 km/s子谱的流量密度呈线性下降趋势,变化时标约为 19天.同时也观测到了整个脉 泽源的谱线宽度与该子谱的强度之间的相关变化.这些现象可能是由脉泽云之间的相 互碰撞导致脉泽抽运率的变化所引起的。  相似文献   

11.
本文作者用澳大利亚Parkes64m射电望远镜观测了OH17.7-2.0的拱星OH脉泽辐射。在观测中共测得了三个峰,其中一个峰是我们新发现的弱源,两个峰是过去发现的强源。用二维Gaussian拟合我们发现强源位置与一个IRAS点源位置相一致,弱源位置在这个IRAS点源位置的西南方。强源的两个峰的速度位置和峰值流量密度都是比较稳定的。  相似文献   

12.
使用澳大利亚Parkes64m射电望远镜,在五个不同的位置上观测了OH17.72.0附近的弱OH脉泽源.发现了一个新的弱OH脉泽源,其峰值速度为52.5km/s.利用二维Gaussian拟合技术,得到了这个源的最佳拟合位置  相似文献   

13.
We analyze our monitoring data for the water-vapor maser in the source W31(2), associated with a region of vigorous star formation, a cluster of OB stars. The monitoring was performed with the 22-m radio telescope at Pushchino Radio Astronomy Observatory during 1981–2004. The variability of the H2O maser in W31(2) was found to be cyclic, with a mean period of 1.9 yr. Two flares were most intense (superflares): in 1985–1986 and 1998–1999. In each activity cycle, we observed up to several short flares, subpeaks. The fluxes of many emission features during the flares were correlated. We also observed successive activation of individual emission features in order of increasing or decreasing radial velocity, suggesting an ordered structure and, hence, a radial-velocity gradient of the medium. There is a clear correlation of the emission peaks of the main components in the spectra at radial velocities of ?1.7, ?1.3, 0.5, and 1.3 km s?1 with activity cycles and of the emission at VLSR < ?8 km s?1 with short flares. During the superflares, the emission in the low-velocity part of the H2O spectrum and a number of other phenomena related to coherent maser-emission properties were suppressed. The maser spots are assumed to form a compact structure, to have a common pumping source, and to be associated with an accretion flow onto the cluster of OB stars.  相似文献   

14.
We have imaged H2O maser emission from the star-forming region S128 at milli-arcsec resolution using MERLIN, to complement 20 years of monitoring data from the Puschino radio telescope. The drift velocities of the masers and the velocity and location of a new maser region add depth to the model of two colliding CO clouds triggering collapse. Some H2O masers appear to originate directly from this shock front. The brightest maser appears typical of a YSO jet and remains unsaturated close to peak intensity. The distribution of maser clumps has a fractal dimension 0.4; combined with analysis of drift velocity variations this suggests that the masers trace the dissipation of supersonic turbulence. The spatial distribution of velocities shows that this is in parts more structured than the Kolmogorov cascade.  相似文献   

15.
We present the results of our observations of the maser radio emission source G188.946+0.886 in hydroxyl (OH) molecular lines with the radio telescope of the Nançay Observatory (France) and in the H2O line at λ = 1.35 cm with the RT-22 radio telescope at the Pushchino Observatory (Russia). An emission feature in the 1720-MHz satellite line of the OH ground state has been detected for the first time. The radial velocity of the feature, V LSR = 3.6 km s?1, has a “blue” shift relative to the range of emission velocities in the main 1665- and 1667-MHz OH lines, which is 8–11 km s?1. This suggests a probable connection of the observed feature in the 1720-MHz line with the “blue” wing of the bipolar outflow observed in this region in the CO line. We have estimated the magnetic field strength for three features (0.90 and 0.8 mG for 1665 MHz and 0.25 mG for 1720 MHz) from the Zeeman splitting in the 1665- and 1720-MHz lines. No emission and (or) absorption has been detected in the other 1612-MHz satellite OH line. Three cycles of H2O maser activity have been revealed. The variability is quasi-periodic in pattern. There is a general tendency for the maser activity to decrease. Some clusters of H2O maser spots can form organized structures, for example, chains and other forms.  相似文献   

16.
We carried out near-infrared imaging observations of the Ori A-W region using the Italian 1.5m TIRGO infrared telescope at Gornergrat. A group of infrared objects is visible on the K band image, including an IRAS source (IRS 1). From its IRAS flux density the IRAS luminosity is derived to be 45L⊙, which shows that IRS 1 is a low-mass protostar. By superimposing the position of the VLA H2O maser on the K image, we can identify the less evolved object IRS 1 as the excitation source of the H2O maser, within a projected distance of 470AU. This would be evidence that the maser effect is associated with the youngest phase of stellar evolution. The first probable HH object candidate in the Ori A-W region is discovered from the H2 S(1) 1-0 observation. Comparing the position of the H2O maser with the direction of the molecular hydrogen emission in the region, we suggest that the observed H2O maser could be tracing the circumstellar disk of IRS 1.  相似文献   

17.
We present the monitoring results for the H2O maser toward the infrared source IRAS 06308+0402 associated with a dense cold molecular cloud. The observations were carried out with the 22-m radio telescope at the Pushchino Radio Astronomy Observatory (Russia) during 1992–2003. The H2O maser was discovered in May 1992 (Pashchenko 1992) during a survey of IRAS sources associated with dense cold clouds with bipolar molecular outflows. The H2O spectrum contains many emission features, suggesting the fragmentation of the envelope around a young star. The star has a low peculiar velocity relative to the CO molecular cloud (~2.2 km s?1). We found a cyclic variability of the total maser flux with a period from 1.8 to 3.1 yr.  相似文献   

18.
We present results of a study of photospheric horizontal motions at the initial and main phases of the solar flare which happened on September 4, 1990, near the solar limb. The flare was accompanied by matter ejection. Spectra of the flare were obtained using the AZU-26 horizontal solar telescope at the MAO NAS (Terskol observatory). We found variations of the matter motion velocity’s value and direction at different stages of the photosphere during the flare development. The velocity changed in a range from −4 to 2 km/s. Comparisons of the obtained data with variations of the chromospheric radial velocities showed that the horizontal matter motions in the photosphere and chromosphere are mostly directed toward the observer but at particular time moments their direction changed. At two different knots, the time shift of the photospheric velocities is different. The highest velocities were observed at the main phase of the flare. At the initial phase of the flare, in the matter ejection region, we note a velocity increase compared with its preflare value and at the flare knots.  相似文献   

19.
We present the results of our study of the H2O maser emission from the source W75N, which is associated with a star-forming region, between November 1994 and March 1999. The observations were carried out with the RT-22 radio telescope of the Pushchino Radio Astronomy Observatory (Lebedev Physical Institute). The maser emission in 1994–1999 can be represented as a superposition of flares of separate components with a duration from two to six months, which occurred mainly in the radial-velocity range 8–17.5 km s?1. We detected a regular drift of the velocity centroid from 13 to 9 km s?1 and an abrupt change in its velocity from 9 to 5 km s?1, which took place at the initial stage of maser activity. Based on the variability of the total H2O flux in all years of our observations of W75N (from December 1979 through March 1999), we conclude that the long-period variability of the water-vapor maser emission has a period of ~11.5 years. We give arguments that this variability is mainly associated with the most compact group of maser spots, whose positions coincide with the position of the continuum source VLA 2.  相似文献   

20.
Using the Nançay radio telescope of Paris Observatory, France, OH 1665 and 1667 MHz masers in the western part of ON2(C) have been observed. The observed emission spectra are analyzed with a thin-disk model, and the positions and Keplerian velocities of the maser spots corresponding to the spectral peaks are obtained.  相似文献   

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