Session S14: Focus Session: Spin Transfer Torque
2:30 PM–4:54 PM, Wednesday, March 7, 2007
Colorado Convention Center Room: Korbel 4D
Sponsoring Units:
GMAG DMP FIAP
Chair: Tom Silva, National Institute of Standards and Technology, Boulder
Abstract ID: BAPS.2007.MAR.S14.7
Abstract: S14.00007 : Spin-Motive Force Studies in Spin-Valves
4:06 PM–4:18 PM
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Abstract 
Authors:
Jun'ichi Ieda
(CREST JST; IMR Tohoku Univ.)
Sadamichi Maekawa
(CREST JST; IMR Tohoku Univ.)
Stewart Barnes
(Physics Dept., Univ. of Miami)
A spin-motive force (smf) is the counterpart of an electro-motive force, which couples to spin degrees of freedom of electrons rather than charge ones. Here we discuss how the smf works in the so-called spin-valves. Usually the observed \textit{dV/dI} for spin-valves is analyzed in terms of magneto-resistance. However when the magnetization makes a sudden jump, there often appears a large peak in \textit{dV/dI}, i.e., a voltage jump that is better interpreted in terms of the smf discussed here. In order to see this, we model spin-valves using an equivalent circuit that involves magnetic dissipation represented by the smf as well as electric dissipation through ordinary resisters for both majority and minority currents. There are four possible conduction paths, e.g., the majority electrons tunnel into the majority band, or into the minority band and vice versa. The first path adds an up electron to the free layer and causes a rotation in a certain sense, while the second path adds a down electron and a rotation in the opposite sense. Since the rotations are in opposite senses so is the work done on the free layer and hence the smf. The equivalent circuit with the relevant parameters predicts a stable large angle precession and the voltage signal.
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2007.MAR.S14.7