论文标题

QPO的纠结磁场模型

Tangled magnetic field model of QPOs

论文作者

Bretz, Joseph, van Eysden, C. A., Link, Bennett

论文摘要

磁铁的高度纠结的磁场支持类似于有序磁场中Alfvén波的剪切波。在这里,我们探讨了在恒星内部和磁层中激发的扭转模式是否可以解释在SGR 1900+14巨型耀斑的尾部观察到的准周期振荡(QPO)。我们解决了一个纠结的磁场的初始值问题,该磁场将内部剪切波融合到磁层中的相对论Alfvén剪切波。假设恒星振荡是由磁能的突然释放而产生的,那么我们获得了该过程的能量和几何形状的约束。如果耀斑能量最初沉积在恒星内,则波能相对缓慢地传播到磁层上,这与观察到的辐射事件的上升时间$ \ \ lyssim 10 $ ms。耀斑能量也不能完全沉积在恒星外面,因为大多数能量反映了恒星表面,从而产生了不足的表面振荡以产生磁层电流的可检测到的调制。跨越恒星表面的体积中的能量沉积与观察到的上升时间一致,并激发了在观察到的QPO频率下具有实质幅度的一系列模式。通常,局部能量沉积激发了包含观察到的QPO的广泛模式,尽管比观察到的QPO的数量更多的模式受到了激发。如果耀斑能量是按轴对称性沉积的,那么对于某些类别的MHD不稳定性可能会大大减少。

The highly tangled magnetic field of a magnetar supports shear waves similar to Alfvén waves in an ordered magnetic field. Here we explore if torsional modes excited in the stellar interior and magnetosphere can explain the quasi-periodic oscillations (QPOs) observed in the tail of the giant flare of SGR 1900+14. We solve the initial value problem for a tangled magnetic field that couples interior shear waves to relativistic Alfvén shear waves in the magnetosphere. Assuming stellar oscillations arise from the sudden release of magnetic energy, we obtain constraints on the energetics and geometry of the process. If the flare energy is deposited initially inside the star, the wave energy propagates relatively slowly to the magnetosphere which is at odds with the observed rise time of the radiative event of $\lesssim 10$ ms. Nor can the flare energy be deposited entirely outside the star, as most of the energy reflects off the stellar surface, giving surface oscillations of insufficient magnitude to produce detectable modulations of magnetospheric currents. Energy deposition in a volume that straddles the stellar surface gives agreement with the observed rise time and excites a range of modes with substantial amplitude at observed QPO frequencies. In general, localized energy deposition excites a broad range of modes that encompasses the observed QPOs, though many more modes are excited than the number of observed QPOs. If the flare energy is deposited axisymmetrically, as is possible for a certain class of MHD instabilities, the number of modes that is excited is considerably reduced.

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