论文标题

在黯然失色的极性BS TRI中积聚

On accretion in the eclipsing polar BS Tri

论文作者

Kolbin, A. I., Borisov, N. V., Serebriakova, N. A., Shimansky, V. V., Katysheva, N. A., Gabdeev, M. M., Shugarov, S. Yu.

论文摘要

我们分析了黯然失色的极性BS TRI的光谱和光度观测。极性的光曲线形状变化可以通过改变积聚流对系统积分辐射的贡献来解释。根据次级辐射部分的径向速度曲线,我们完善了系统组件的质量,$ m_1 = 0.60 \ pm 0.04 m _ {\ odot} $,$ m_2 \ $ m_2 \ of 0.12 m _ {\ odot} $ {\ odot} $,以及orbital conciritian concipin and counce concipin and $ i = 85 = 85 = 85 = 85 = 85^^\ pm {5.5^^^^\ c {5^5^^^。极性光谱揭示了在积聚点形成的回旋谐波,磁场强度为$ b = 22.7 \ pm 0.4 $ mg,平均温度为$ t \ sim 10 $ keV。除了回旋谐波外,BS TRI光谱还包含H $α$线的Zeeman组件,它们可能是在积聚点附近的凉晕中形成的。通过对极性的光曲线进行建模,可以估算磁偶极子和吸积点的坐标的方向。我们表明,要对BS〜TRI光曲线进行满意的描述,我们必须考虑到沿视线的光学深度的可变性。 BS TRI的多普勒地图显示了积聚流的一部分,其轨迹接近Lagrange Point l $ _1 $附近的弹道,而该流的另一部分则沿着磁场线移动。从多普勒断层图中发现的停滞区域位置的估计与吸积斑位置的光度估计一致。

We analyze spectroscopic and photometric observations of the eclipsing polar BS Tri. The polar's light curve shape variations can be interpreted by changing contributions of the accretion stream to the integral radiation of the system. Based on the radial velocity curves of the irradiated part of the secondary, we refine the masses of the system components, $M_1 = 0.60 \pm 0.04 M_{\odot}$, $M_2 \approx 0.12 M_{\odot}$, and the orbital inclination, $i=85\pm 0.5^{\circ}$. The polar's spectra reveal cyclotron harmonics forming in an accretion spot with a magnetic field strength of $B=22.7 \pm 0.4$ MG and an average temperature of $T \sim 10$ keV. In addition to the cyclotron harmonics, the BS Tri spectra contain Zeeman components of H$α$ line, which are probably formed in the cool halo near the accretion spot. The orientation of the magnetic dipole and the coordinates of the accretion spot are estimated by modeling the light curves of the polar. We show that for a satisfactory description of the BS~Tri light curves we have to take into account the variability of the spot's optical depth along the line of sight. Doppler maps of BS Tri show a part of the accretion stream with a trajectory close to ballistic near the Lagrange point L$_1$, and another part of the stream moving along the magnetic field lines. The estimate of the stagnation region position found from the Doppler tomograms is consistent with the photometric estimates of the accretion spot position.

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