共查询到20条相似文献，搜索用时 140 毫秒
1.
A.J. Willis Luc Dessart P.A. Crowther P.W. Morris K.A. Van Der Hucht 《Astrophysics and Space Science》1997,255(1-2):167-168
We have obtained ISO SWS spectroscopy of WR 146 (WC6+O) covering the wavelength range 2.6-20 μm. WC6 wind emission is observed
in numerous lines of He II and C IV, as well as in the [Ne III] 15.5 μm line, but not in [Ne II] 12.81 or [Ne V] 14.32 μm.
An analysis of these spectra (and complementary radio and optical data) yields for the WC6 star: v∞ = 2700 km s-1; M=2.6×10-5M⊙yr-1;
C/He = 0.15; and a neon abundance bound of 3.4×10-3≤Ne/He≤6.8×10-3. The neon abundance is close to that predicted in stellar
evolution models of WC stars.
This revised version was published online in August 2006 with corrections to the Cover Date. 相似文献
2.
HE1005-1439是一颗金属丰度极低([Fe/H] ~ - 3.0)的碳增丰贫金属星(Carbon Enhanced Metal-Poor,CEMP), 该星的s-过程元素显著超丰([Ba/Fe] = 1.16±0.31, [Pb/Fe] = 1.98±0.19), 而r-过程元素温和超丰([Eu/Fe] = 0.46±0.22), 使用单一的s-过程模型和i-过程模型均不能拟合该星中子俘获丰度分布. 采用丰度分解的方法探究该星化学元素的天体物理来源可有助于理解CEMP星的形成和化学演化. 利用s-过程和r-过程的混合模型对其中子俘获元素的丰度分布进行拟合, 发现该星的中子俘获元素主要来源于低质量低金属丰度AGB伴星的s-过程核合成, 而r-过程核合成也有贡献. 相似文献
3.
SDSSJ022119.84＋005628.4： A Radio-Loud Narrow-LineSeyfert 1 Galaxy with Star Formation in its Nucleus
Jing Wang Jian-Yan Wei Xiang-Tao He Department of Astronomy Beijing Normal University Beijing National Astronomical Observatories Chinese Academy of Sciences Beijing 《中国天文和天体物理学报》2004,4(5):415-426
The optical spectrum of SDSS J022119.84 + 005628.4 (R. A. = 02h 21m 19.84s, Dec = 00°56' 28.4", J2000; z = 0.399785 ± 0.000558) is analyzed by multi-component profile modelling. The small flux ratio of [OⅢ]NC/Hβ (=0.78) and FWHM(HβBC) = 1778.1 ±85.9 km s-1 led us to identify SDSS J022119.84 + 005628.4 as a Narrow-line Seyfert 1 galaxy with RFe= 1.4-1.0+1.0 and intermediate radio loudness, logR = 1.93. The continuum low jump at the Balmer limit might be contributed by a starburst component, which suggests that the object is a relatively young AGN with star-formation activity in its inner region. This provides a useful observational test of the AGN evolution. The low flux ratio of the narrow components, [OⅢ]/Hβ = 1.62, and the prominent [OⅡ]γ3727 emission, [OⅡ]/[OⅢ] = 2.24, suggests that there should be a group of AGNs different from Seyfert 2s when their broad line regions are obscured by the torus on the line of sight. A possible orientation effect is suggested to interpret the observed Seyf 相似文献
4.
赵刚 《中国天文和天体物理学报》1993,(4)
本文确定了贫金属矮星和亚巨星的重元素丰度.基于高分辨率高信噪比光谱得到27颗样本星的锶、钇、锆、钡、镧、铈和铕丰度.主要结果为:(1)第一峰区元素锶-钇-锆显示了奇偶效应,在晕族星中钇相对于锶和锆过贫。(2)对[Fe/H]>-2.5的恒星钇丰度为常数([Y/Fe]=-0.06).(3)对于[Fe/H]<-1.7的样本星,随金属丰度减小钡过贫增加·(4)镧和铈相对于铁过贫.(5)在金属丰度-1.0>[Fe/H]>- 2.0 区间,铕表现过富.(6)对[Y/Fe],[Zr/Fe]和[Ba/Fe]存在约0.1dex的本质弥散. 相似文献
5.
本文叙述了以下内容: (1)对在1963年5月18日到8月8日拍摄的7条武仙座1963年新星的光谱作了发射带相对强度的测定(表2)。 (2)按新星光度变化的统计规律得到上述新星的距离模数值(10~m),用平均消光法求得目视总吸光值A_v=0~m.23,距离900秒差距,井由此得到改正星际选择吸光后的谱带的相对强度(表3)。 (3)由新星绝对星等M_B和发射带的相对强度求得了谱带的绝对强度(表4)。 (4)对于一些发射带的绝对强度作Δm-lgt图,发现发射带绝对强度的变化也存在Δm=blgt的线性关系。对于不同的谱线,系数b是不同的。 (5)根据测定的相对强度,用安巴楚勉和斯托伊两种方法求得核星温度,它们分别在150000°—160000°和30000°—60000°之间,由于前者是上限,后者是下限,真实的核星温度应当在两种方法求得的值之间。 (6)用H_β的绝对强度和[OⅢ]5007+4959对[OⅢ]4363的强度比两种方法分别求得不同电子温度T_e相对应的电子密n_e。并且用由上述两个方法求得的T_e—n_e曲线的交点,同时求得了T_e和n_e的值。由此法求得的结果是:在所讨论的期间内,T_e由10800°K逐渐上升到17500°K,然后又下降至13000°K。n_e则单调的由5.0×10~7cm~(-3)逐渐下降到7.0×10~6cm~(-3)。 (7)求得壳层质量约为2.3×10~(-5)M_⊙。 (8)初步分析了一些壳层物理参数变化的原因。 相似文献
6.
本文利用文[1]和文[2]所给出的高红移类星体吸收系统的证认方法,对目前最大红移类星体QS02000-330(z_e=3.78)的吸收光谱进行了吸收线红移系统的证认,并得到了六个重元素的吸收线系统:z_a=3.1881,3.1913,3.3335,3.5519以及z_a=1.3441,3.3459。前四个系统和Hunstead等人(1986)所得到的A、B、C、D系统(红移值分别是z_a=3.1881,3.1914,3.3332,3.5519)相符合;后两个是我们新发现的吸收系统。 相似文献
7.
8.
广义相对论中静态荷电球体的一组内解 总被引：1，自引：0，他引：1
李鉴增 《中国天文和天体物理学报》1983,(3)
本文在假定物质密度ρ_m=μr~α,电荷密度 ρ_e=ρ_0r~βe~(-λ/2)的情况下,严格求解 Einstein-Maxwell 场方程,得出了静态荷电球体的一组内解,把文[4]、[6]的结果作为自己的特例包括在内。 相似文献
9.
《天文和天体物理学研究(英文版)》2016,(7)
The [α/Fe] ratios in stars are good tracers to probe the formation history of stellar populations and the chemical evolution of the Galaxy. The spectroscopic survey of LAMOST provides a good opportunity to determine [α/Fe] of millions of stars in the Galaxy. We present a method of measuring the [α/Fe]ratios from LAMOST spectra using the template-matching technique of the LSP3 pipeline. We use three test samples of stars selected from the ELODIE and MILES libraries, as well as the LEGUE survey to validate our method. Based on the test results, we conclude that our method is valid for measuring [α/Fe]from low-resolution spectra acquired by the LAMOST survey. Within the range of the stellar parameters Teff= [5000, 7500] K, log g = [1.0, 5.0] dex and [Fe/H]= [onsistent with values derived from high-resolution spectra,-1.5, +0.5] dex, our [α/Fe] measurements are c and the accuracy of our [α/Fe] measurements from LAMOST spectra is better than 0.1 dex with spectral signal-to-noise higher than 20. 相似文献
10.
《天文和天体物理学研究(英文版)》2015,(8)
Most Galactic metal-poor stars exhibit enhanced α-abundances(e.g.[Mg/Fe] ～ +0.4) according to previous studies of stellar chemical compositions.However, a handful of metal-poor stars with large deficiencies in Mg(e.g. [Mg/Fe]～-0.2) show severe departures from this α-enhancement trend. The sub-solar[Mg/Fe] ratios of these anomalous stars indicate that they possess different chemical enrichment histories than the majority of Galactic metal-poor stars. In previous work,we presented a method to select Mg-poor metal-poor stars from low-resolution SDSS spectra based on a spectral matching technique. In this paper, a similar method is applied to low-resolution(R ～ 1800) LAMOST spectra. Stellar [Mg/Fe] abundances are determined by using stellar parameters delivered by the LAMOST Data Release2 catalog. From a sample of ～ 60 000 stars with atmospheric parameters in the range Teff = [5500, 6500] K and [Fe/H] = [-2.4, +0.5], we select 15 candidate Mg-poor metal-poor stars. 相似文献
11.
塞佛特星系ＮＧＣ1 0 6 8是一个非常令人注目的特殊天体 ,它是Ｓｅｙｆｅｒｔ[1]发现的第一批此类星系中离我们最近 (1 9Ｍｐｃ,取Ｈ0 =6 0ｋｍｓ- 1Ｍｐｃ- 1)和最亮的一个塞佛特星系 ,因此天文学家从射电到Ｘ 射线整个电磁波段对它进行了详尽的观测和研究。ＮＧＣ1 0 6 8最初被归类为塞佛特ＩＩ型天体 ,但是通过对其偏振光的光谱观测 ,发现了认为被遮挡住的塞佛特Ｉ型核发出的± 432 0ｋｍ/ｓ的宽Ｈβ发射线 ,因此被认为是活动星系核统一模型的一个范例 (见文 [2 ] )。射电与光学的观测资料都表明ＮＧＣ1 0 6 8的中心部分有激烈的喷射活动… 相似文献
12.
We performed an extensive non-LTE analysis of the neutral sodium lines of Na I 5683/5688, 5890/5896, 6154/6161, and 8183/8195 in disk/halo stars of types F-K covering a wide metallicity range (-4 (?) [Fe/H] (?) +0.4), using our own data as well as data collected from the literature. For comparatively metal-rich disk stars (-1(?) [Fe/H] (?) +0.4) where the weaker 6154/6161 lines are the best abundance indicators, we confirmed [Na/Fe]- 0 with an "upturn" (i.e., a shallow/broad dip around -0.5 (?) [Fe/H](?) 0) as already reported in previous studies. For the metal-deficient halo stars, where the much stronger 5890/5896 or 8183/8195 lines subject to considerable (negative) non-LTE corrections amounting to 0.5 dex have to be used, our analysis suggests mildly "subsolar" [Na/Fe] values down to--0.4 (with a somewhat large scatter of-±0.2 dex) on the average at the typical halo metallicity of [Fe/H] --2, followed by a rise again to a near-solar ratio of [Na/Fe] - 0 at the very metal-poor regime [Fe/H]--3 to -4 相似文献
13.
本根据金星空间探测器对金星重力场的最新探测结果，讨论了由于金星重力场的非对称性引起的对金星自转演化中的影响。计算结果表明，金星自转速率具有周期性变化为：·/ω=1.751×10^-18sin2[(ι ωt)=7°.33]根据金星内部构成的模型力学性质，计算了上式引起的金星的永久变形，从而导致其对自转轴惯性矩的变化。根据[1]的结论，金星形成初期为快速顺向自转的天体，取其平均初始自转周期T0＝15小时，则可求得其自转速率的长期减慢为：·/ωg=-6.2155×10^-22弧度／秒^2。如果金星形成后其重力场的变化不大，那么由图1结果可知·/ωg对金星初期的自转速率变化曾起过一定的作用。 相似文献
14.
《天文和天体物理学研究(英文版)》2016,(1)
We aim at deriving accurate atmospheric parameters and chemical abundances of 19 barium(Ba) stars, including both strong and mild Ba stars, based on the high signal-to-noise ratio and high resolution Echelle spectra obtained from the 2.16 m telescope at Xinglong station of National Astronomical Observatories, Chinese Academy of Sciences. The chemical abundances of the sample stars were obtained from an LTE, plane-parallel and line-blanketed atmospheric model by inputting the atmospheric parameters(effective temperatures Teff, surface gravities log g, metallicity [Fe/H] and microturbulence velocity ξt) and equivalent widths of stellar absorption lines. These samples of Ba stars are giants as indicated by atmospheric parameters, metallicities and kinematic analysis about UVW velocity. Chemical abundances of 17 elements were obtained for these Ba stars. Their Na, Al, α- and iron-peak elements(O, Na, Mg, Al, Si, Ca,Sc, Ti, V, Cr, Mn, Ni) are similar to the solar abundances. Our samples of Ba stars show obvious overabundances of neutron-capture(n-capture) process elements relative to the Sun. Their median abundances of[Ba/Fe], [La/Fe] and [Eu/Fe] are 0.54, 0.65 and 0.40, respectively. The Y I and Zr I abundances are lower than Ba, La and Eu, but higher than the α- and iron-peak elements for the strong Ba stars and similar to the iron-peak elements for the mild stars. There exists a positive correlation between Ba intensity and [Ba/Fe].For the n-capture elements(Y, Zr, Ba, La), there is an anti-correlation between their [X/Fe] and [Fe/H]. We identify nine of our sample stars as strong Ba stars with [Ba/Fe]0.6 where seven of them have Ba intensity Ba=2-5, one has Ba=1.5 and another one has Ba=1.0. The remaining ten stars are classified as mild Ba stars with 0.17[Ba/Fe]0.54. 相似文献
15.
Yoichi Takeda Gang Zhao Masahide Takada-Hidai Yu-Qin Chen Yu-ji Saito Hua-Wei Zhang 《中国天文和天体物理学报》2003,3(4):316-340
We performed an extensive non-LTE analysis of the neutral sodiumlines of Na I 5683/5688, 5890/5896, 6154/6161, and 8183/8195 in disk/halo starsof types F-K covering a wide metallicity range (-4 [Fe/H] +0.4), using ourown data as well as data collected from the literature. For comparatively metal-rich disk stars (-1 [Fe/H] +0.4) where the weaker 6154/6161 lines are thebest abundance indicators, we confirmed [Na/Fe] ～ 0 with an "upturn" (i.e., ashallow/broad dip around -0.5 [Fe/H] 0) as already reported in previousstudies. For the metal-deficient halo stars, where the much stronger 5890/5896 or8183/8195 lines subject to considerable (negative) non-LTE corrections amountingto 0.5 dex have to be used, our analysis suggests mildly "subsolar" [Na/Fe] valuesdown to ～ -0.4 (with a somewhat large scatter of ～±0.2 dex) on the average at thetypical halo metallicity of [Fe/H] ～ -2, followed by a rise again to a near-solar ratioof [Na/Fe] ～ 0 at the very metal-poor regime [Fe/H] ～ -3 to -4. These resultsare discussed in comparison with the previous observational studies along with thetheoretical predictions from the available chemical evolution models. 相似文献
16.
Da-Ming ChenNational Astronomical Observatories Chinese Academy of Sciences Beijing cdm@bao.ac.cn 《中国天文和天体物理学报》2004,4(2):118-124
We investigate the linear amplitude of mass fluctuations in the universe, σ8, and the present mass density parameter of the Universe, Ωm, from statistical strong gravitational lensing. We use the two population model of lens halos with fixed cooling mass scale Mc = 3×1013h-1M⊙ to match the observed lensing probabilities, and leave σ8 orΩm as a free parameter to be constrained by the data. Another varying parameter, the equation of state of dark energy ω, and its typical values of -1, -2/3, -1/2 and -1/3 are investigated. We find that σ8 is degenerate with Ωm in a way similar to that suggested by present day cluster abundance as well as cosmic shear lensing measurements: σ8Ω0.6m≈0.33. However, both σ8≤0.7 and Ωm≤0.2 can be safely ruled out, the best fit is when σ8 = 1.0, Ωm = 0.3 and ω= - 1. This result is different from that obtained by Bahcall & Bode, who gave σ8 = 0.98±0.1 and Ωm = 0.17 ±0.05. For σ8 = 1.0, the higher value ofΩm = 0.35 requires ω = -2/3 and Ωm = 0.40 require 相似文献
17.
本文简略介绍了一种新的六极型铯束管的结构和性能。新就新在它不用电子倍增器,而是采用高阻放大器(计置院研制),这就在我国首次成功地解决了铯束管长寿命工作中的一个关键问题.束光学用“点源”“点靶”轴对称地配置获得了如下的电参数:Ramseg 谐振信号:9×10~(-12)ARamseg 谐振线宽:190Hz信噪比(平均时间1秒):583铯炉工作温度(℃):95与中国计量科学院研制的线路配合,获得了如下的整机参数:频率稳定度:δg(τ=1h)=1.9×10~(11)/τ~(1/2)[δy(τ=1h)=3.3×10~(-13)]频率准确度:±7×10~(-12)(数据尚不充分)今后再做适当的改进.不难将稳定度提高到1～2×10~(-13)/h,它完全有希望成为我们国产的能长期(1年以上)连续运行的高性能的铯束频标。在国际上,六极型的铯束装置在联邦德国物理技术研究院(PTB)得到了极其成功的应用,该实验室已完成了准确度高达1～2×10~(-14)作用区短到0.8米的铯束频率基准,苏联和日本也研制成功了类似的装置。 相似文献
18.
本文分析了1982年10月——1983年5月期间YLF的SPA事件的数据和太阳x—射线爆发资料.并且和文献[1]中LF的SPA事件的分析作了比较。可以看出,VLF的SPA事件和太阳x—射线爆发有较好的相关性;在1—8埃频段的太阳x—射线爆发能产生VLF的SPA事件的门限值为1×10~(-6)Wm~(-2).这个值比LF的SPA事件的门限值(2×10~(-6)Wm~(-2))要低一倍. 相似文献
19.
Ke-Feng Sun Ji Yang Shao-Guang Luo Min Wang Li-Cai Deng Xu Zhou Jian-Sheng Chen Department of Astronomy Peking University Beijing sunkf Chinese Academy of Sciences-Peking University Joint Beijing Astrophysical Center Beijing Purple Mountain Observatory Chinese Academy of Sciences Nanjing National Astronomical Observatories Chinese Academy of Sciences Beijing 《中国天文和天体物理学报》2003,3(5):458-468
We report our new results on Herbig-Haro (HH) objects in the star forming region of Taurus from a wide-field survey with the 60/90 cm Schmidt telescope of the Beijing Astronomical Observatory. This survey using CCD imaging with a narrow band [SII] filter and an intermediate band [BATC10] filter covered approximately 30 square degrees in Taurus. Besides confirming the known HH Objects in the region, we discovered seven new HH candidates, and groups. Six of these are HH 701A-B, HH 702A-D, HH 703, HH 704A-D, HH 705, HH 706 and the seventh is a group, a new component of HH 319, labeled HH 319B-D. Based on the large-scale distribution of pre-main-sequence (PMS) stars in Taurus, we analyze statistically the most probable distance from the HH objects to each PMS star, from which we estimate the typical timescale of these HH objects to be between (1.3 - 2.0) ×104 yrs; and we also obtain the birth rates of HH objects: 0.447±0.198 for Class Ⅰ PMS stars, 0.360±0.222 for Class Ⅱ PMS stars, and -0.148±0.234 fo 相似文献
20.
《天文和天体物理学研究(英文版)》2015,(8)
We have compared stellar parameters, including temperature, gravity and metallicity, for common stars in the LAMOST DR2 and SDSS DR12/APOGEE datasets. It is found that the LAMOST dataset provides a more well-defined red clump feature than the APOGEE dataset in the Teff versus log g diagram. With this advantage, we have separated red clump stars from red giant stars, and attempt to establish calibrations between the two datasets for the two groups of stars. The results show that there is a good consistency in temperature with a calibration close to the one-to-one line, and we can establish a satisfactory metallicity calibration of[Fe/H]APOGEE= 1.18[Fe/H]LAMOST + 0.11 with a scatter of ～ 0.08 dex for both the red clump and red giant branch samples. For gravity, there is no correlation for red clump stars between the two datasets, and scatters around the calibrations of red giant stars are substantial. We found two main sources of scatter in log g for red giant stars. One is a group of stars with 0.00253 × Teff- 8.67 log g 2.6 located in the forbidden region, and the other is the contaminated red clump stars, which could be picked out from the unmatched region where stellar metallicity is not consistent with position in the Teff versus log g diagram. After excluding stars in these two regions,we have established two calibrations for red giant stars, log g APOGEE = 0.000615 ×Teff,LAMOST+ 0.697 × log g LAMOST- 2.208(σ = 0.150) for [Fe/H] -1 and log gAPOGEE= 0.000874×Teff,LAMOST+0.588×log g LAMOST-3.117(σ = 0.167)for [Fe/H] -1. The calibrations are valid for stars with Teff = 3800- 5400 K and log g = 0- 3.8 dex, and are useful in work aiming to combine the LAMOST and APOGEE datasets in a future study. In addition, we find that an SVM method based on asteroseismic log g is a good way to greatly improve the accuracy of gravity for these two regions, at least in the LAMOST dataset. 相似文献