Paper MI-ThM2
Dependence of the Domain Wall Pinning Strengths to Lateral Constriction Size and Electrical Bias in GaMnAs
Thursday, November 12, 2009, 8:20 am, Room C1
Session: |
Magnetization Dynamics, Imaging and Spectroscopy |
Presenter: |
S.U. Cho, Seoul National University, Korea |
Authors: |
S.U. Cho, Seoul National University, Korea H.K. Choi, Seoul National University, Korea Yang, Seoul National University, Korea Park, Seoul National University, Korea F. DaSilva, National Institute of Standards and Technology T. Osminer, National Institute of Standards and Technology D.P. Pappas, National Institute of Standards and Technology |
Correspondent: |
email address not available |
Dynamics of domain wall (DW) motion and spin-polarized transport across DWs have received much attention due to their potential applications in large-scale memory storage and logic devices. Particularly for GaMnAs, spin-polarized current induced magnetization switching has been demonstrated [1]. Lateral nanoconstrictions (NC), from which DWs can form and be pinned, in GaMnAs have been utilized to demonstrate nonvolatile memory elements [2] as well as structures showing large magneto-resistances (MRs) [3]. Here, we investigate the size dependence of constrictions in GaMnAs epifilms, particularly the dependence of DW pinning strength as function of lateral constriction size, as well as electrical bias across the constriction. A method to realize nanoconstrictions without plasma-assisted methods and nonlinear IV transport across NC junctions have been reported previously [4]. For this study, we present magnetotransport measurements on identically sized constrictions in series (up to five NC in series) equally spaced apart (~ 2 microns). For large constrictions, the overall resistance (<25 kΩ at room temperature) as function of applied field shows a background negative MR response which can be attributed to anisotropic magnetoresistance with distinct jump-down behavior. The number of distinct jump-down behavior corresponds to number of NC plus one with little dependence of jump field to bias current. Thus, for large constrictions, the geometrical lateral constrictions act ‘to seed’ DWs. For smaller constrictions (overall resistance > 25 kΩ at room temperature), the MR response is more complex as DW are formed and pinned at the lateral constrictions. MR responses show jump-up behavior along with a complex dependence on jump field to bias current. Furthermore, we will discuss the complex switching behavior observed in small constrictions in series in terms of effects attributed to DW motion and spin-polarized transport across DWs.
[1] M. Yamanouchi et al., Nature 428, 539 (2004).
[2] K. Rappert et al., Nat. Phys. 3, 573 (2007).
[3] C. Rüster et al., Phys. Rev. Lett. 91, 216602 (2003); A.D. Giddings et al., Phys. Rev. Lett. 94, 127202 (2005).
[4] S.U. Cho et al. Appl. Phys. Lett. 91, 122514 (2007).