Piezo-control of magnetic anisotropy in GaMnAs: Reversible manipulation of magnetization orientation and irreversible magnetization switching
| dc.creator | Bihler, C. | |
| dc.creator | Althammer, M. | |
| dc.creator | Brandlmaier, A. | |
| dc.creator | Gepraegs, S. | |
| dc.creator | Weiler, M. | |
| dc.creator | Opel, M. | |
| dc.creator | Schoch, W. | |
| dc.creator | Limmer, W. | |
| dc.creator | Gross, R. | |
| dc.creator | Brandt, M. S. | |
| dc.creator | Goennenwein, S. T. B. | |
| dc.date | 2008-04-08 | |
| dc.date.accessioned | 2026-07-07T09:49:16Z | |
| dc.date.available | 2026-07-07T09:49:16Z | |
| dc.description | We have investigated the magnetic properties of a piezoelectric actuator/ferromagnetic semiconductor hybrid structure. Using a GaMnAs epilayer as the ferromagnetic semiconductor and applying the piezo-stress along its [110] direction, we quantify the magnetic anisotropy as a function of the voltage V_p applied to the piezoelectric actuator using anisotropic magnetoresistance techniques. We find that the easy axis of the strain-induced uniaxial magnetic anisotropy contribution can be inverted from the [110] to the [1-10] direction via the application of appropriate voltages V_p. At T=5K the magnetoelastic term is a minor contribution to the magnetic anisotropy. Nevertheless, we show that the switching fields of rho(H) loops are shifted as a function of V_p at this temperature. At 50K - where the magnetoelastic term dominates the magnetic anisotropy - we are able to tune the magnetization orientation by about 70 degree solely by means of the electrical voltage V_p applied. Furthermore, we derive the magnetostrictive constant lambda_111 as a function of temperature and find values consistent with earlier results. We argue that the piezo-voltage control of magnetization orientation is directly transferable to other ferromagnetic/piezoelectric hybrid structures, paving the way to innovative multifunctional device concepts. As an example, we demonstrate piezo-voltage induced irreversible magnetization switching at T=40K, which constitutes the basic principle of a nonvolatile memory element. | |
| dc.identifier | https://arxiv.org/abs/0804.1336 | |
| dc.identifier | http://arxiv.org/abs/0804.1336 | |
| dc.identifier | Phys. Rev. B 78, 045203 (2008) | |
| dc.identifier | doi:10.1103/PhysRevB.78.045203 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/164524 | |
| dc.subject | Materials Science | |
| dc.title | Piezo-control of magnetic anisotropy in GaMnAs: Reversible manipulation of magnetization orientation and irreversible magnetization switching | |
| dc.type | text |