共查询到19条相似文献，搜索用时 125 毫秒
1.
为解释Ｂｅ／Ｘ射线双星波段联合观测结果，已发展了许多理论模型。在本文中简述这些Ｂｅ／Ｘ射线双星理论模型的研究现状，包括枞两个正常的Ｂ型星组成的密近双星演化成为Ｂｅ／Ｘ射线双星的演化模型，描述Ｂｅ星气壳的物理模型，Ｂｅ星和中子星的性质所决定的中子星吸积方式的吸积量及Ｂｅ／Ｘ射线双星Ｘ射线源光变曲线的理论解释。 相似文献
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简要地回顾了Ｂｅ／Ｘ射线双星２０多年来在红外、可见光、紫外和Ｘ射线波段所取得的观测结果，着重介绍了多波段联合观测对探讨双星间的相互作用如中子星的吸积方式和Ｘ射线产生的原因等方面的意义，对这些观测结果的分析研究，将是人们了解Ｂｅ／Ｘ射线双星的轨道参数和双星的物理参数、建立理论模型的基础。 相似文献
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对ＸＰｅｒ新发射相连续四年的光学光谱和近红外光度监测结果，ＸＰｅｒ近两年的变化不同寻常，主要表现以下两点：（１）尽管它的光学光度Ｖ星等只恢复至失去气壳前的亮度，但Ｈａ发射线等值宽度和近红外，Ｊ，Ｈ和Ｋ光度地超过了历史记录的最大值，分别达到了１６．３４Ａ和５．３＾ｍ，５．３＾ｍ和５．１＾ｍ，表明ＸＰｅｒ新发射相气南的密度和尺度较都大，（２）我们首次观测到ＸＰｅｒ近红外光度和Ｈα发射线等值宽度变化趋势 相似文献
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介绍了Ｂｅ星的基本特性，评术字近年来对Ｂｅ星星周物质结构研究的成果，重点介绍了最亲的关于Ｂｅ星星周周产生和变化的动力不模型，另外，对Ｂｅ／Ｘ射线双星系统的研究了做了简评述，重点论述了致密层与Ｂｅ星延伸大气的相互作用。 相似文献
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本文详细讨论了Ｘ射线双星ＣｙｇＸ－３的Ｘ光子场对γ射线的吸收效应，计算结果表明：当ＣｙｇＸ－３的Ｘ光子发射场处于高态时，从致密中子星附近发射的能量为１０＾２－１０＾４ＭｅＶ的γ射线约有６０％被其吸收，吸收过程产生的正负电子的逆Ｃｏｍｐｔｏｎ散射会使出射能量１０－７０ＭｅＶ的 γ射线强度平均增加约５０％，计算的γ射线能谱与实验观测结果基本相符。 相似文献
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小质量Ｘ射线双星在６－７ｋｅＶ的铁发射线具有一些明显观测特征，如谱线展宽、红移和轮廓非对称性。这些性质可能是由高价Ｆｅ离子发射线光子穿过致密天体周围较“冷”等离子体介质时的康普软化过程所造成，本文按此模型求解了康普软化扩散方程，所得理论谱线轮廓与观测线拟合得很好。拟合参量（等离子体的汤姆孙散射光深）取为τｅ～３，由此定出散射等离子体电子密度Ｎｅ≈１０＾１６ｃｍ＾－３，散射球半径Ｒ≈１０＾９ｃｍ． 相似文献
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Ｂe单星和Ｂe／Ｘ射线双星作为一类特殊早型天体和特殊的大质量Ｘ射线双星,在各个波段都有与其它相同光谱型的Ｂ型天体显著不同的特征,因此长期以来引起中外天文学者的关注。首先在可见光波段发射线的存在,就是对仅产生吸收线的经典大气的挑战;其次Ｂe星作为一类早型带有包层天体,研究Ｂe星包层的性质,对研究原恒星包层性质和进一步了解早 型星其它光谱型的性质是非常重要的;再者可以研究Ｂe星的存在与星际磁场或湍流的星际 相似文献
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本文收集了ＳＭＭ运行期间（１９８０．２－１９８９．１１）与地面观测相对应的太阳白光耀斑ＨＸＲＢＳ和ＧＲＳ观测资料，就白光耀斑与硬Ｘ－射线发射及伽玛射线发射之产的关系进行了初步的统计研究，结果表明：白光耀斑与伽玛射线发射之间不存在对应关系；白光耀斑也并非全具有强硬Ｘ－射线发射，对那些只具有对较弱的硬Ｘ－射线发射的白光耀斑，我们发现低能粒子具有足够的能量驱动连续发射，因而它们可能起源于色球，而对那些具 相似文献
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本文采用相对论微扰法处理Ｆｅ（＋２４）系统，利用解析形式的波函数计算其低能态的能级结构及Ｋα、Ｋβ特征线（作为对比，我们也计算了Ｆｅ（＋２５）系统）．通过与现有的Ｆｅ（＋２５）Ｋα线的实验和理论比较，证明我们的方法是准确可信的，而在数学计算上则更加简便。利用这一结果，对小质量Ｘ射线密近双星的Ｆｅ（＋２４）Ｋ特征线进行了简要的定性分析． 相似文献
10.
王建民 《紫金山天文台台刊》1999,18(3):271-273
频繁的超新星爆发可用以解释活动星系核与类星体的超高金属丰度。星团中的恒星与吸积盘相互作用导致致密天体中子星和黑洞的形成率很高,这些致密天体与红巨星很容易形成双星系统,而后形成（ＮＳ／ＢＨ,ＮＳ／ＢＨ） 双星由于引力辐射最终导致并合而形成伽玛射线爆发。我们估计了伽玛射线爆的爆发频率,发现与观测相符。 相似文献
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We present a series of optical spectroscopic andnear-infrared photometric observations of the Be star X Persei, from thebeginning of the recent emission phase. Our data show that after the latestextended low state (ELS), both the equivalent width (EW) of theH emission line and the JHK luminosities gradually increased. Therecent maximum H EW and JHK magnitudes are more than butcomparable to the 1986–1989 maxima, which reflects a more extensiveand denser envelope in the new emission phase.The IR photometry and the H EW increase coincidently in theearly stage of the new emission phase. However, the variations in thefollowing years, especially in 1994 and 1995, are much different from theearly trend. An unusual variation that while the H EW in X Perincreases considerably, the JHK magnitudes decline rapidly is seen in ournearly simultaneous spectroscopic and near-infrared observations.An expanding ring model is put forward to interpret the observedunusual variation between the H EW and near-IR luminosity duringthe recent emission phase of X Persei. Our results indicate that althoughboth infrared excess and H emission line arise from the envelope,their main contributors, in some cases, are likely to originate in thedifferent part of the envelope. 相似文献
12.
J. S. Clark I. A. Steele M. J. Coe & P. Roche 《Monthly notices of the Royal Astronomical Society》1998,297(3):657-666
We present infrared spectroscopy of the Be/X-ray binary HDE 245770/A0535+26 obtained over the period 1992–1995. The spectra show significant variability, reflecting changes in the circumstellar environment during this time. A reduction in the flux observed in the Paschen series lines between 1993 December and 1994 September correlates with a similar reduction in both the strength of Hα and the optical continuum emission, which can be attributed to a reduction in the emission measure of the disc. A turnover between optically thin and thick emission is seen for both Paschen and Brackett series lines, and allows an estimate of the disc density as ∼1012 cm−3 . Echelle spectroscopy reveals strong similarities between the He I 1.008, 2.058 μm, Hα and Paschen series line profiles, suggesting their formation in a similar (and asymmetric) region of the disc. In contrast, the line profile of He I 6678 Å indicates that it is formed at smaller radii than the other transitions. 相似文献
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Krishna M. V. Apparao S. P. Tarafdar R. P. Verma K. V. K. Iyengar K. K. Ghosh 《Journal of Astrophysics and Astronomy》1993,14(3-4):131-134
The observed infrared excess in Be stars is usually interpreted as free-free and free-bound emission from a hot gas envelope
around the Be star. This hot gas should also emit H-alpha line radiation. Earlier observations had suggested that the infrared
excess and Hα radiation were not consistent with models in which they arise from the same ionized region; however the observations
were made at different times. We have made simultaneous observation of infrared and H-alpha line radiation. Our observations
imply that either both these radiations cannot arise from the same hot gas or additional processes have to be invoked to account
for the observed excess infrared radiation. 相似文献
14.
We present results of near infrared observation of 21 molecular outflow sources and two non-outflow sources with compact cores. Combined with IRAS and other surface station observations we analyse their spectra and find that the outflow sources have, on average, steeper spectral gradients than the non-outflow sources in the range 2.28–25 μ. Most of the bipolar outflow sources have gradients greater than 2.0. Using a revised blackbody photosphere model we calculate the contributions to the JHK fluxes by the central young star and the circumstellar envelope. For the sources with known bolometric luminosity we derive the photospheric temperature of the central star and the circumstellar extinction. Results show that most of the young stars associated with molecular outflows are probably T Tauri stars (5000–7000 K) or emission line stars (9000–26000 K). The circumstellar extinction in JHK is around 10 to 20 magnitudes. These facts show that molecular outflow sources are young objects still embedded deep inside or around the interior of compact cores. Fitting the 3.5– 25 μ and 60–100 μ spectra with a λ-1 dust emission model to five source gives a negative power law for the temperature profile of the circumstellar shell with exponents between 0.39 and 0.48, close to the theoretical results for molecular clouds associated with HI I regions. 相似文献
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We collected almost all Galactic Wolf-Rayet (hereafter WR) stars found so far from the literature. 578 WR stars are gathered in this paper. 2MASS counterparts with good quality magnitudes in all JHK bands are listed for 364 WR stars. In addition, WISE counterparts for these sources are also identified. It is found that free-free emission is the main dominant source for the infrared excess in most WR stars up to 3.4 μm. However at the longer wavelengths the thermal radiation is dominant. In addition, WR stars in Clusters of the Galactic center region have the strong infrared excess in the near infrared due to the dust thermal emission from the strong star forming activity in the Galactic center region. For some WR stars with the WC spectral type, in particular, with WCd type, the dust thermal emission is important radiation source while many WR stars with the WC spectral type have the near infrared flux enhancement from the broad line emission in the K band. It is also shown that many single WC stars with different spectral sub-types have different locations in the near infrared two-color diagram, in particular, WC6 and WC9d stars can be separated respectively from other spectral type stars while single WN stars with different spectral sub-types can not be separated in the near infrared two-color diagram. 相似文献
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《New Astronomy Reviews》1999,43(8-10):563-567
The masers in three stars, S Per, OH53.6-0.2 and VXSgr, were observed in the main lines of OH at λ18 cm in March 1997 with a VLBI array consisting of 6 EVN antennas and 3 in the USA. Both S Per and VX Sgr were detected on transatlantic baselines, showing that at least some of the maser spots are very compact with sizes less than around 2 mas. The observations confirm that in S Per there is main line OH emission close to star at a similar distance (≈ 100 AU) as the H2O shell. The most blue-shifted emission comes from the centre of the object suggesting radial amplification of the maser radiation, whilst most of the remainder comes from a thick shell, some 100 AU from the star. This contrasts with the 1612 MHz OH emission that comes from an outer shell some 1000 AU from the star. Estimates of the magnetic fields in the shell from Zeeman pairs in S Per show fields of a few hundred nT. 相似文献