Heide C
Department of Physics, New York University, 4 Washington Place, New York, New York 10003, USA.
Phys Rev Lett. 2001 Nov 5;87(19):197201. doi: 10.1103/PhysRevLett.87.197201. Epub 2001 Oct 22.
Spin currents injected into magnetic thin films may noticeably change the magnetization of the films. To describe this effect, exchange coupled Landau-Lifshitz equations for the local magnetization and the spin-polarized charge carriers are combined with transport equations for charge and spin currents. For steady state transport one obtains two different instability conditions. Both conditions are supported by recent experimental data on current induced magnetization reversal and spin-wave excitations. No second ferromagnetic layer is needed for excitations due to spin transfer.
注入磁性薄膜的自旋电流可能会显著改变薄膜的磁化强度。为描述这种效应,将用于局部磁化强度和自旋极化电荷载流子的交换耦合朗道-里夫希茨方程与电荷和自旋电流的输运方程相结合。对于稳态输运,可得到两种不同的不稳定性条件。这两种条件均得到了关于电流诱导磁化反转和自旋波激发的最新实验数据的支持。由于自旋转移激发不需要第二个铁磁层。