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Magnetic field structure and accretion regimes of the asynchronous polar BY Cam

机译:异步极性BY Cam的磁场结构和吸积方式

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摘要

Series of photometric CCD observations of the asynchronous polar BY Cam in a low accretion state (R = 14(m)-16(m)) were made on the K-380 telescope at the Crimean Astrophysical Observatory (CrAO) over 100 hours in the course of 31 nights during 2004-2005. A period of P-1 = 0.137120 +/- 0.000002 days was found for the variations in the brightness, along with less significant periods of P-2 = 0.139759 +/- 0.000003 and P-3 = 0.138428 +/- 0.000002 days, where P-2 and P-3 are obviously the orbital and rotation periods, while the dominant period P-1 is the sideband period. A modulation in the brightness and an amplitude of 0.137 days in the oscillations at the orbital-rotational beat period (synodic cycle) of 14.568 +/- 0.003 day are found for the first time. The profile of the modulation period is four humped. This indicates that the magnetic field has a quadrupole component, which shows up well during the low brightness state. Accretion takes place simultaneously into two or three accretion zones, but at different rates. The times of the times of maxima for the main accretion zone vary with the phase of the beat period. Three types of variation of this sort are distinguished: linear, discontinuous, and chaotic, which indicate changes in the accretion regimes. At synodic phases 0.25 and 0.78 the bulk of the stream switches by 180 degrees, and at phase 0.55, by similar to 75 degrees. At phases of 0.25-0.55 and 0.55-0.78, the O-C shift with a period of 0.1384 days, which can be explained by a retrograde shift of the main accretion zone relative to the magnetic pole and/or a change in the angle between the field lines and the surface of the white dwarf owing to the asynchronous rotation. For phases of 0.78-1.25 the motion of the accretion zone is quite chaotic. It is found that synchronization of the components occurs at a rate of less than dP(rot)/P-rot similar to 10(-9) day/day.
机译:在克里米亚天体观测站(CrAO)的K-380望远镜上,在100个小时内对低极化状态(R = 14(m)-16(m))的异步极地偏光凸轮进行了一系列的光度CCD观测。在2004年至2005年的31个晚上。发现亮度变化的时间段为P-1 = 0.137120 +/- 0.000002天,P-2 = 0.139759 +/- 0.000003和P-3 = 0.138428 +/- 0.000002天的显着性时间段较小,其中P-2和P-3显然是轨道和自转周期,而主导周期P-1是边带周期。首次发现在14.568 +/- 0.003天的轨道旋转节拍周期(共鸣周期)的振荡中亮度调制和振幅为0.137天。调制周期的轮廓是四个峰。这表明磁场具有四极分量,该分量在低亮度状态下表现良好。吸积同时进入两个或三个吸积区,但速率不同。主吸积区的最大时间随拍频周期的相位而变化。可以区分出三种类型的变化:线性变化,不连续变化和混沌变化,它们表明了吸积方式的变化。在共生阶段0.25和0.78时,大部分物流转换180度,而在阶段0.55转换约75度。在0.25-0.55和0.55-0.78阶段,OC偏移为0.1384天,这可以用主吸积区相对于磁极的逆行偏移和/或磁场之间的角度变化来解释。线和白矮星的表面由于异步旋转。对于0.78-1.25的相位,吸积区的运动非常混乱。已经发现,组件的同步发生的速率小于dP(rot)/ P-rot,类似于10(-9)天/天。

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