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再发新星船底座PY星的远紫外光谱学

FAR ULTRAVIOLET SPECTROSCOPY OF THE RECURRENT NOVA T PYXIDIS.

作者信息

Godon Patrick, Sion Edward M, Starrfield Sumner, Livio Mario, Williams Robert E, Woodward Charles E, Kuin Paul, Page Kim L

机构信息

Astronomy & Astrophysics, Villanova University, Villanova, PA 19085, USA.

School of Earth and Space Exploration, Arizona State University, Tempe, AZ 85287, USA.

出版信息

Astrophys J Lett. 2014 Apr 1;784(No 2). doi: 10.1088/2041-8205/784/2/L33. Epub 2014 Mar 19.

DOI:10.1088/2041-8205/784/2/L33
PMID:29430290
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC5804888/
Abstract

With six recorded nova outbursts, the prototypical recurrent nova T Pyxidis (T Pyx) is the ideal cataclysmic variable system to assess the net change of the white dwarf mass within a nova cycle. Recent estimates of the mass ejected in the 2011 outburst ranged from a few 10 to 3.3 × 10, and assuming a mass accretion rate of 10-10 yr for 44 yr, it has been concluded that the white dwarf in T Pyx is actually losing mass. Using NLTE disk modeling spectra to fit our recently obtained COS and STIS spectra, we find a mass accretion rate of up to two orders of magnitude larger than previously estimated. Our larger mass accretion rate is due mainly to the newly derived distance of T Pyx (4.8 kpc, larger than the previous 3.5 kpc estimate), our derived reddening of ( - ) = 0.35 (based on combined and spectra), and NLTE disk modeling (compared to blackbody and raw flux estimates in earlier works). We find that for most values of the reddening (0.25 ≤ (-) ≤ 0.50) and white dwarf mass (0.70 ≤ ≤ 1.35 ) the accreted mass is larger than the ejected mass. Only for a low reddening (0.25 and smaller) a large white dwarf mass (0.9 and larger) is the ejected mass larger than the accreted one. However, the best results are obtained for a larger value of reddening.

摘要

作为典型的再发新星,北冕座T星(T Pyx)有六次记录在案的新星爆发,是评估新星周期内白矮星质量净变化的理想激变变星系统。近期对2011年爆发时抛出物质质量的估计范围在约10到3.3×10之间,假设在44年里吸积率为10-10 年,得出的结论是北冕座T星中的白矮星实际上在损失质量。利用非局部热动平衡盘模型光谱来拟合我们最近获得的COS和STIS光谱,我们发现吸积率比之前估计的大两个数量级。我们得出的更大吸积率主要归因于新测定的北冕座T星距离(4.8千秒差距,大于之前估计的3.5千秒差距)、我们得出的色指数(-)=0.35(基于组合的和光谱)以及非局部热动平衡盘模型(与早期工作中的黑体和原始流量估计相比)。我们发现,对于大多数色指数值(0.25≤(-)≤0.50)和白矮星质量值(0.70≤≤1.35 ),吸积的质量大于抛出的质量。只有在低色指数(约0.25及更小)和大白矮星质量(0.9及更大)的情况下,抛出的质量才大于吸积的质量。然而,对于更大的色指数值能得到最佳结果。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/249b/5804888/d091d0f1bbb8/nihms938787f5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/249b/5804888/d185ebe616cb/nihms938787f1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/249b/5804888/bd5412dcea4d/nihms938787f2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/249b/5804888/7ef253644cba/nihms938787f3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/249b/5804888/376b37c0c65f/nihms938787f4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/249b/5804888/d091d0f1bbb8/nihms938787f5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/249b/5804888/d185ebe616cb/nihms938787f1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/249b/5804888/bd5412dcea4d/nihms938787f2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/249b/5804888/7ef253644cba/nihms938787f3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/249b/5804888/376b37c0c65f/nihms938787f4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/249b/5804888/d091d0f1bbb8/nihms938787f5.jpg

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