快速旋转中间极性 CTCV J2056-3014 的宽带 X 射线研究

Ciro Salcedo, Kaya Mori, Gabriel Bridges, Charles J. Hailey, David A. H. Buckley, Raimundo Lopes de Oliveira, Gavin Ramsay and Anke van Dyk
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摘要

我们报告了XMM-Newton、NuSTAR和NICER对CTCV J2056-3014的X射线观测结果。CTCV J2056-3014是一个大灾变变星(CV),它是自旋速度最快的白矮星(WD)之一,自旋周期为P = 29.6秒。虽然CJ2056以前被归类为中极性变星,但它也表现出了WZ Sge型CV的特性,例如矮新星和超级爆发。通过XMM-牛顿和NICER,我们探测到了∼2 keV的自旋周期,其意义为7σ。在对双星轨道运动进行校正后,我们将其导数约束为 s s-1。脉冲轮廓的特征是一个宽峰,调制率为 25%。NuSTAR探测到未被吸收的X射线通量增加了四倍,这与2022年11月的一次光学耀斑相吻合。XMM-牛顿和NICER在0.310keV的X射线光谱最适合吸收、光学稀薄的三温热等离子体模型(kT=0.3、1.0和4.9keV),而NuSTAR在3-30keV的光谱最适合单温热等离子体模型(kT=8.4keV),两者的铁丰度ZFe/Z⊙=0.3。CJ2056 与其他快速旋转的 CV 有着相似之处,如等离子体温度较低,在低能量时没有明显的 X 射线吸收。由于 WD 的磁场强度未知,我们采用了非磁性和磁性 CV 光谱模型(MKCFLOW 和 MCVSPEC)来确定 WD 的质量。得出的 WD 质量范围(M = 0.7-1.0 M⊙)高于离心分裂质量极限 0.56 M⊙,并且与当地 CV 的平均 WD 质量(M ≈ 0.8-0.9 M⊙)一致。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
A Broadband X-Ray Investigation of Fast-spinning Intermediate Polar CTCV J2056–3014
We report on XMM-Newton, NuSTAR, and NICER X-ray observations of CTCV J2056–3014, a cataclysmic variable (CV) with one of the fastest-spinning white dwarfs (WDs) at P = 29.6 s. While previously classified as an intermediate polar, CJ2056 also exhibits the properties of WZ Sge–type CVs, such as dwarf novae and superoutbursts. With XMM-Newton and NICER, we detected the spin period up to ∼2 keV with 7σ significance. We constrained its derivative to s s−1 after correcting for binary orbital motion. The pulse profile is characterized by a single broad peak with ∼25% modulation. NuSTAR detected a fourfold increase in unabsorbed X-ray flux coincident with an optical flare, in 2022 November. The XMM-Newton and NICER X-ray spectra at 0.310 keV are best characterized by an absorbed, optically thin three-temperature thermal plasma model (kT = 0.3, 1.0, and 4.9 keV), while the NuSTAR spectra at 3–30 keV are best fit by a single-temperature thermal plasma model (kT = 8.4 keV), both with Fe abundance ZFe/Z⊙ = 0.3. CJ2056 exhibits similarities to other fast-spinning CVs, such as low plasma temperatures and no significant X-ray absorption at low energies. As the WD’s magnetic field strength is unknown, we applied both nonmagnetic and magnetic CV spectral models (MKCFLOW and MCVSPEC) to determine the WD mass. The derived WD mass range (M = 0.7–1.0 M⊙) is above the centrifugal breakup mass limit of 0.56 M⊙ and consistent with the mean WD mass of local CVs (M ≈ 0.8–0.9 M⊙).
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