排序方式： 共有115条查询结果，搜索用时 15 毫秒
31.
W. Pietsch 《Astronomische Nachrichten》2008,329(2):170-173
First studies of the X‐ray source population of M 31 were performed with the Einstein Observatory and ROSAT. High resolution Chandra Observatory images not only spatially resolved the center area but also supernova remnants (SNRs) in the galaxy. Source catalogues of restricted areas were presented with high astrometric accuracy. Also luminosity function studies and studies of individual sources based on Chandra and XMM‐Newton observations led to a better knowledge of the X‐ray source population. An XMM‐Newton source catalog based on archival observations revealed more than 850 sources down to a 0.2–4.5 keV luminosity of 1035 erg s–1. EPIC hardness ratios as well as informations from earlier X‐ray, optical, and radio catalogues were used to distinguish between different source classes (SNRs, supersoft sources (SSSs), X‐ray binaries (XRBs), globular cluster sources within M 31, and foreground stars and objects in the background). However, many sources could only be classified as “hard”. These sources may either be XRBs or Crab‐like SNRs in M 31 or background sources. Two of the globular cluster sources could be identified as low mass XRBs with a neutron star as compact object as they showed type I X‐ray bursts. Many of the SSSs were identified as optical novae. Inspired by these results an XMM‐Newton survey of the entire D25 disk of M 31 and a dedicated program to monitor X‐ray counterparts of optical novae in M 31 was started. We discuss implications for further nearby galaxy studies. (© 2008 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim) 相似文献
32.
33.
Jun Ma Richard de Grijs Zhou Fan Soo-Chang Rey Zhen-Yu Wu Xu Zhou Jiang-Hua Wu Zhao-Ji Jiang Jian-Sheng Chen Kyungsook Lee Sangmo Tony Sohn 《中国天文和天体物理学报》2009,9(6)
Mayall Ⅱ = G1 is one of the most luminous globular clusters (GCs) in M31. Here, we determine its age and mass by comparing multicolor photometry with theo-retical stellar population synthesis models. Based on far- and near-ultraviolet GALEX photometry, broad-band UBV RI, and infrared JHK8 2MASS data, we construct the most extensive spectral energy distribution of G1 to date, spanning the wavelength range from 1538 to 20000A. A quantitative comparison with a variety of simple stellar pop-ulation (SSP) models yields a mean age which is consistent with G1 being among the oldest building blocks of M31 and having formed within ～1.7Gyr after the Big Bang. Irrespective of the SSP model or stellar initial mass function adopted, the resulting mass estimates (of order 107M⊙) indicate that G1 is one of the most massive GCs in the Local Group. However, we speculate that the cluster's exceptionally high mass suggests that it may not be a genuine GC. Our results also suggest that G1 may contain, on average, (1.65±0.63) × 102L⊙ far-ultraviolet-bright, hot, extreme horizontal-branch stars, depend-ing on the adopted SSP model. In addition, we demonstrate that extensive multi-passband photometry coupled with SSP analysis enables one to obtain age estimates for old SSPs that have similar accuracies as those from integrated spectroscopy or resolved stellar pho-tometry, provided that some of the free parameters can be constrained independently. 相似文献
34.
35.
KSS31M型海洋重力仪在动、静态条件下观测到的读数变化及分析 总被引：3，自引：3，他引：0
2002年中国科学院海洋研究所从德国引进了KSS31M型海洋重力仪．为对该重力仪的工作性能有详细的了解,分别在德国重力仪生产厂实验室、中国科学院海洋研究所重力仪实验室进行了静态的定点观测,将重力仪安装在考察船上在黄埔江渔政码头等地进行了动态条件下的定点观测．动、静态的定点观测发现了多种规律性的重力仪读数变化,分析认为这些规律性的读数变化分别是重力仪的随机振荡、月潮的重力效应、海潮的重力效应和重力仪的线性漂移．它们各自有着不同的变化规律,并在海洋重力观测时总是同时存在．重力仪的随机振荡是重力仪自身固有的,其振荡幅度随外界条件的变化而变化,一般为0．04mGal～0．5mGal,周期为2～5min不等,在德国的重力仪厂家实验室和中国科学院海洋研究所重力实验室中观测到了月潮引起的重力变化,其变化幅度为0．2mGal．月潮引起的重力变化和海潮引起的重力变化同步,但相位相反．本文指出,仪器的月漂往往很难精确判定,本文用多种方法计算得到的仪器月漂在1．2mGal到2．3mGal之间． 相似文献
36.
37.
38.
39.
J. Ma R. de Grijs Y. Yang X. Zhou J. Chen Z. Jiang Z. Wu J. Wu 《Monthly notices of the Royal Astronomical Society》2006,368(3):1443-1450
We independently redetermine the reddening and age of the globular cluster (GC) 037−B327 in M31 by comparing independently obtained multicolour photometry with theoretical stellar population synthesis models. 037−B327 has long been known to have a very large reddening value, which we confirm to be E ( B − V ) = 1.360 ± 0.013 , in good agreement with the previous results. We redetermine its most likely age at 12.4 ± 3.2 Gyr .
037−B327 is a prime example of an unusually bright early counterpart to the ubiquitous 'super' star clusters presently observed in most high-intensity star-forming regions in the local Universe. In order to have survived for a Hubble time, we conclude that its stellar initial mass function (IMF) cannot have been top-heavy. Using this constraint, and a variety of simple stellar population (SSP) models, we determine a photometric mass of , somewhat depending on the SSP models used, the metallicity and age adopted and the IMF representation. This mass, and its relatively small uncertainties, makes this object the most massive star cluster of any age in the Local Group. Assuming that the photometric mass estimate thus derived is fairly close to its dynamical mass, we predict that this GC has a (one-dimensional) velocity dispersion of the order of (72 ± 13) km s−1 . As a surviving 'super' star cluster, this object is of prime importance for theories aimed at describing massive star cluster evolution. 相似文献
037−B327 is a prime example of an unusually bright early counterpart to the ubiquitous 'super' star clusters presently observed in most high-intensity star-forming regions in the local Universe. In order to have survived for a Hubble time, we conclude that its stellar initial mass function (IMF) cannot have been top-heavy. Using this constraint, and a variety of simple stellar population (SSP) models, we determine a photometric mass of , somewhat depending on the SSP models used, the metallicity and age adopted and the IMF representation. This mass, and its relatively small uncertainties, makes this object the most massive star cluster of any age in the Local Group. Assuming that the photometric mass estimate thus derived is fairly close to its dynamical mass, we predict that this GC has a (one-dimensional) velocity dispersion of the order of (72 ± 13) km s
40.
We derive the constraints on the mass ratio for a binary system to merge in a violent process. We find that the secondary-to-primary stellar mass ratio should be 0.003 ≲ ( M 2 / M 1 ) ≲ 0.15 . A more massive secondary star will keep the primary stellar envelope in synchronized rotation with the orbital motion until merger occurs. This implies a very small relative velocity between the secondary star and the primary stellar envelope at the moment of merger, and therefore very weak shock waves, and low-flash luminosity. A too low-mass secondary will release small amount of energy, and will expel small amount of mass, which is unable to form an inflated envelope. It can, however, produce a quite luminous but short flash when colliding with a low-mass main-sequence star.
Violent and luminous mergers, which we term mergebursts, can be observed as V838 Monocerotis-type events, where a star undergoes a fast brightening lasting days to months, with a peak luminosity of up to ∼106 L⊙ followed by a slow decline at very low effective temperatures. 相似文献
Violent and luminous mergers, which we term mergebursts, can be observed as V838 Monocerotis-type events, where a star undergoes a fast brightening lasting days to months, with a peak luminosity of up to ∼10