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arXiv 1007.3859cond-mat.mtrl-sci
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自旋力矩纳米接触涡旋振荡器的功率谱理论

Theory of the power spectrum of spin-torque nanocontact vortex oscillators

Joo-Von Kim, Thibaut Devolder

摘要:

磁性纳米接触中的自旋转移力矩可以导致涉及大振幅回旋涡旋运动的自持磁化振荡。这种动力学包括围绕纳米接触的稳态轨道,这是可能的,因为固有的磁阻尼由自旋扭矩补偿。在这篇文章中,我们提出了一个分析理论,这些振荡的功率谱的基础上的刚性涡模型。在nanocontacts的涡旋振荡的外观是不相关的霍普夫分岔:没有临界电流和在有限电流的稳态振荡的唯一先决条件是在系统中的涡旋的存在,与传统的自旋扭矩振荡器,涉及大角度磁化进动。振荡频率与外加电流成线性关系,与轨道半径成反比。通过求解涡旋动力学的朗之万问题,得到了功率谱的线形和线宽。在典型的实验条件下,一个洛伦兹线型与电流无关的线宽进行了预测。良好的定量之间的理论和最近的实验。

英文摘要:

Spin-transfer torques in magnetic nanocontacts can lead to self-sustained magnetization oscillations that involve large-amplitude gyrotropic vortex motion. This dynamics consists of a steady state orbit around the nanocontact, which is made possible because the intrinsic magnetic damping is compensated by spin torques. In this article, we present an analytical theory of the power spectrum of these oscillations based on a rigid-vortex model. The appearance of vortex oscillations in nanocontacts is not associated with a Hopf bifurcation: there is no critical current and the only precondition for steady-state oscillations at finite currents is the existence of a vortex in the system, in contrast with conventional spin-torque oscillators that involve large-angle magnetization precession. The oscillation frequency is found to depend linearly on the applied current and inversely proportional to the orbital radius. By solving the associated Langevin problem for the vortex dynamics, the lineshape and linewidth for the power spectrum are also obtained. Under typical experimental conditions, a Lorentzian lineshape with a current-independent linewidth is predicted. Good quantitative agreement between the theory and recent experiments is shown.

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