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1.
大质量分子云核的CO同位素搜寻   总被引:1,自引:0,他引:1  
使用紫金山天文台 13.7 m望远镜上新安装的 SIS系统,对 64个高色指数 IRAS源和水脉泽源进行了 CO同位素13CO和 C18O J= 1-0的搜寻,并对部分源作了成图观测.结果在 64个源中全部测到了这一谱线对,而13CO的辐射一般较强,说明与稠密分子区成协,其中约60个源为首次作CO同位素谱线对巡测.用高斯拟会导出了天线温度、线心速度和谱线全半宽.对辐射强度、话线特征进行了初步分析.  相似文献   

2.
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   

3.
L1498 is a classic example of a dense cold pre-protostellar core. To study the evolutionary status, the structure, dynamics, and chemical properties of this core we have obtained high spatial and high spectral resolution observations of molecules tracing densities of 10(3)-10(5) cm-3. We observed CCS, NH3, C3H2, and HC7N with NASA's DSN 70 m antennas. We also present large-scale maps of C18O and 13CO observed with the AT&T 7 m antenna. For the high spatial resolution maps of selected regions within the core we used the VLA for CCS at 22 GHz, and the Owens Valley Radio Observatory (OVRO) MMA for CCS at 94 GHz and CS (2-1). The 22 GHz CCS emission marks a high-density [n(H2) > 10(4) cm -3] core, which is elongated with a major axis along the SE-NW direction. NH3 and C3H2 emissions are located inside the boundary of the CCS emission. C18O emission traces a lower density gas extending beyond the CCS boundary. Along the major axis of the dense core, CCS, NH3 and C3H2 emission show evidence of limb brightening. The observations are consistent with a chemically differentiated onion-shell structure for the L1498 core, with NH3 in the inner and CCS in the outer parts of the core. The high angular resolution (9"-12") spectral line maps obtained by combining NASA Goldstone 70 m and VLA data resolve the CCS 22 GHz emission in the southeast and northwest boundaries into arclike enhancements, supporting the picture that CCS emission originates in a shell outside the NH3 emitting region. Interferometric maps of CCS at 94 GHz and CS at 98 GHz show that their emitting regions contain several small-scale dense condensations. We suggest that the differences between the CCS, CS, C3H2, and NH3 emission are caused by a time-dependent effect as the core evolves slowly. We interpret the chemical and physical properties of L1498 in terms of a quasi-static (or slowly contracting) dense core in which the outer envelope is still growing. The growth rate of the core is determined by the density increase in the CCS shell resulting from the accretion of the outer low-density gas traced by C18O. We conclude that L1498 could become unstable to rapid collapse to form a protostar in less than 5 x 10(6) yr.  相似文献   

4.
We present results of 13CO(1-0),C18O(1-0),and HCO+(1-0) map observations and N2H+(1-0) single point observations directed towards a sample of nine low-luminosity 6.7-GHz masers.N2H + line emission has been detected from six out of nine sources,C18O line emission has been detected from eight out of nine sources,and HCO + and 13CO emission has been detected in all sources.In particular,a blue profile of the HCO + spectrum,a signature of inflow,is found towards one source.From integrated intensity emission map...  相似文献   

5.
本文作者首次对暗云L1211的C~(18)O(J=1-0)分子发射谱线进行了观测,发现了暗云L1211致密核的C~(18)O(J=1-0)的宽翼发射谱线和它的结构,得到了核区C~(18)O(J=1-0)分子的谱线轮廓图、强度分布图、速度分段积分等高图、速度位置图。  相似文献   

6.
利用紫金山天文台青海观测站13.7米的毫米波望远镜对74个大质量年轻星体或候选进行了C^18O(1-0)的谱线观测。在63个源中观测到了C^18O(1-0)发射,其中57个天体第一次探测到C^18O(1-0)谱线发射。根据谱线辐射温度(TR^*)和半宽(△V),利用LTE方法计算了每个测量源的C^18O(1-0)发射的光学厚度和C^18O(1-0)分子的柱密度。讨论了^13CO(1-0)和C^18O(1-0)的谱线强度比和积分强度比。  相似文献   

7.
With the 13.7 m millimeter wave telescope of Purple Mountain Observatory at Qinghai Station, the simultaneous mapping observations at the 12CO(J=1-0), 13CO(J=1-0) and C18O(J=1-0) lines were performed towards the 24 Galactic high-mass star-forming cores, which are associated with water masers and have available Spitzer's infrared data. The average mapping range was 8′ × 8′. The C18O line emission was detected in all the cores, in which 11 cores were observed to the half maximum of their C18O integrated intensities and the rather extended (5′ − 8′) C18O maps were obtained, while the others were failed to make such a large scale mapping because of the low SNR or the intrinsically extended morphology of the cores. On the 11 completely mapped dense cores, we analyzed their characteristics and made the statistics and comparisons on the integrated intensity ratios between 12CO and 13CO (R12/13), 13CO and C18O(R13/18), as well as 12CO and C18O(R12/18). We concluded that as a tracer of dense gas, C18O is absolutely optically thin and can be used to detect the detailed structures of the cores, and that in general the 3 ratios increase gradually from the core center to the periphery. We found that the integrated intensity ratio R12/13 ranges from 2 to 6; R13/18 fluctuates between 4 and 20, but in central regions it is concentrated in the range 6–12 with a small fluctuation; and R12/18 occupies a wider range 13–90, but it is concentrated between 13 and 50 in the denser regions of the cores.  相似文献   

8.
We map the dark molecular cloud core of L134 in the C18O (J = 1 - 0) emission line using the PMO 13.7m telescope, and present a contour map of integrated intensity of C18O (J = 1 - 0) emission. The C18O cloud is inside the distribution of extinction AB, the visual extinction of blue light, as well as inside the 13CO cloud in the L134 region. The depletion factors in this C18O cloud are generally greater than unity, which means there is gas depletion onto dust. Since only a minimum AB = 9.7 mag is available, and our observations measure both undepleted and depleted regions along the line of sight, the depletion factors could very likely be larger in the central core than the calculated value. So we conclude that depletion does occur in the bulk of the C18O cloud through a comparison between the C18O and blue extinction maps in the L134 region. There is no direct evidence as yet for star formation in L134, and so cores on the verge of collapse will not be visible in CO and other gas molecules.  相似文献   

9.
The distribution of dense molecular gas around the supernova remnant G40.5-0.5 has been investigated by radio spectroscopic observations in the CO (J = 1-0) transition. The molecular gas is found to extend over the entire region of G40.5-0.5. A molecular shell, with a diameter of - 26', coincides with the ionized gas as revealed by the cm-radio observations. This coincidence, along with the velocity discontinuity following the shell, provides direct evidence for interaction between the ionized gas and the dense molecular gas. No clear evidence for cosmic-ray acceleration can be identified from this SNR as previously suggested, due to positional uncertainty in relating the SNR shell defined by CO to the EGRET gamma-ray sources, GRO J1904 06, from the gamma-ray observations.  相似文献   

10.
New J=1-0 HCO+ and J=2-1 C18O observations of HH24–26 reveal striking differences between these and previous maps of higher-J transitions of HCO+ and CS. The high-J HCO+ and CS emission traces the densest portions of the cloud, while C18O traces the more tenuous envelope. This is also evident in the velocity structure. HCO+ and C18O appear to be depleted from the gas phase by amounts which vary with position.  相似文献   

11.
恒星形成于分子云之中, 分子外向流是恒星形成正在进行的重要动力学特征, 也是研究和认识恒星形成的重要契入点. 利用紫金山天文台青海观测站德令哈13.7m毫米波望远镜, 采用5种分子谱线探针(包括12CO、13CO、C18O、HCO$^+$ $J=1-0$和CS $J=2-1$, J为角动量量子数), 对一个包含IRAS 19230+1506、IRAS 19232+1504和G050.3179--00.4186这3个源的大质量恒星形成复合体进行了成图观测研究. 通过对以上分子谱线数据并结合红外波段巡天数据的分析, 在这3个源中首次探测到了分子外向流活动, 并确定了分子外向流的中心驱动源. 最后对这3个源进行了分子外向流相关物理量参数的计算, 分析了这些物理量参数之间的关系, 结果表明分子外向流的性质与中心驱动源的性质息息相关.  相似文献   

12.
吴月芳  韩溥 《天文学报》1998,39(3):244-250
用紫金山天文台青海观测站13.7米毫米波望远镜新安装的3毫米系统,对一组包括大质量恒星形成区、稠密云核、Bok球、主序前发射线星和演化晚期恒星的源进行了12COJ=1-0的辐射搜寻.结果在不同质量恒星形成区域全部测到了12CO辐射,并发现了大的线宽、红和蓝的线翼、线心速度变化及多重辐射的特征,表明相应源可能具有双极喷流,存在膨胀、旋转或多核斑结构.有两个演化晚期星中已观测到了12COJ=1-0谱线,说明其具有较浓厚的拱星气体包层.  相似文献   

13.
在红外天文卫星点源表中选取了具有陡远红外谱的97个源及其它8个红外源,用射电天文联合实验室紫金山天文台青海站的137m望远镜,进行了CO(J=1-0)的观测.结果在102个源中测到了CO辐射,有9个源参考位置难以确定,21个源有多重成分,在其余72个源中有29个具有高速气体,其中18个是新测到的双极外向流候选者,对其性质及与年轻星体的关系作了简要讨论.  相似文献   

14.
俞志尧 《天文学报》1998,39(4):405-411
从在CepheusE中C18O(J=1-0)的谱线频谱图发现,相对于峰速度的蓝移成分的积分流量密度明显大于相对于红移成分的积分流量密度.从在它的强度分布图也可以发现强度分布轮廓向西北和向东延伸.为此,研究了在CepheusE中C18O(J=1-0)的速度分段积分等高图,发现相对于峰速度的蓝移速度分段积分等高图中的C18O(J=1-0)的积分强度,要大于相对于红移速度分段积分等高图中的C18O(J=1-0)的积分强度,同时强度分布图中的分子外流的不准直分布是由相对于峰速度的蓝移成分的分布的不准直性所引起的.  相似文献   

15.
We report the astronomical detections of several ammonia inversion transitions involving nonmetastable levels with energies as high s 1090 K above the ground state. The (J, K) = (9, 6) inversion transition shows maser-like emission in the directions of W51, NGC 7538, W49, and DR 21(OH). The NH3 (6, 3) line exhibits similar characteristics in W51 but is seen in absorption in NGC 7538. These are the first definite detections of ammonia masers in space. The intensities and narrow line widths (0.5-1.5 km s-1) for the emission features are in contrast to the previously detected broad, weak, nonmetastable lines attributed to thermal emission in these sources. Temporal variability appears to be evident in the (9, 6) emission in W49 over a 4 month period. The highly excited (J, K) = (9, 6) and (6, 3) ammonia lines are found in regions containing compact H II regions and strong infrared sources with associated H2O and OH masers; i.e., in regions of active star formation.  相似文献   

16.
利用日本名古屋大学天体物理系的毫米波射电望远镜对CepheusC的C18O(J=1-0)分子辐射首次进行了观测,得到了强度分布图.从强度分布图上,我们发现C18O(J=1-0)分子的分布呈现三个核.通过计算得到了三个核的物理参数.  相似文献   

17.
HCO+ has been detected for the first time towards the star Cygnus OB2 No. 12 through emission of the 1–0 rotational transition at 89 GHz. The CO( J =2−1) transition has also been observed. The observations are consistent with a model of dense regions embedded in a low-density clump gas. If actually present, the dense component would have an aggregate size L 1300 au, in agreement with estimates of small-scale density fluctuations observed along diffuse lines of sight.  相似文献   

18.
We present observations of the 1300 micron continuum emission and the C18O spectral-line emission from three well-studied giant molecular cloud cores: Orion, W49, and W51. The observations were obtained at the Five College Radio Astronomy Observatory, and they provide a means to examine the consistency of these two methods to trace the column density structure of molecular clouds. We find a good general correlation between the 1300 micron continuum, which traces the column density of dust, and the C18O J = 2 --> 1 line emission, which traces the column density of molecular gas, when the effects of source temperature are taken into consideration. Moreover, nominal values for the gas and dust abundances and the dust properties reproduce the observed continuum-to-line ratios. Thus, no strong C18O abundance gradients within sources has been found, and it appears that either the C18O emission lines or the submillimeter dust emission may be used to derive the mass column density within molecular clouds accurately.  相似文献   

19.
SiS has been conclusively detected toward Orion-KL via its J = 6-5 and J = 5-4 rotational transitions at 91 and 109 GHz. Line profiles indicate that the species is present at an LSR velocity of 7.5 km s-1 with a half-width at zero power of 36 km s-1. Such characteristics associate SiS with the moderate velocity outflow (V approximately 18 km s-1) centered on IRc2 and observed in thermal SiO, the NH3 "plateau," and OH, H2O, and SiO masers. The column density estimated for SiS in this region is Ntot = 4 x 10(15) cm-2, corresponding to a fractional abundance of f approximately 4 x 10(-9). Such an abundance implies an SiO/SiS ratio of approximately 60 in the outflow material, remarkably close to the cosmic O/S ratio of approximately 40 and contrasting with the SiO/SiS value of > approximately 10(3) predicted by ion-molecule models. This difference is probably a result of the high temperatures and densities present in the outflow, which favor thermal equilibrium abundances similar to those observed in the circumstellar shells of late-type stars rather than "ion-molecule"-type concentrations. In addition to SiS, some twenty new unidentified lines near 91 and 109 GHz were detected toward KL, as well as transitions arising from HC5N, HC13CCN, HCC13CN, O13CS, and, possibly, CH3CH2OH, CH3CHO, and CH3OD.  相似文献   

20.
We present CS(J = 1 0) observations of the high density gas in a sample of eleven star forming regions with molecular or optical outflows. The sources of this sample cover a wide range of physical sizes. All these sources had been previously mapped in NH3 (1,1) with similar angular resolution. In all the sources of this sample CS emission was detected, indicating a global correlation between the emissions traced by the CS and the NH3 molecules. However, the detailed characteristics of these two emissions (e.g., the extent and the location of the emission peak) show, in general, significant differences in the sources which are well resolved by the beam. As a general trend, the emission traced by the NH3 molecule appears as compact clumps which engulf an outflow activity center. In contrast, the emission traced by the CS molecule, usually more extended, appears as a background which connects different outflow activity centers associated with each NH3 clump.  相似文献   

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