Memory effect and temperature behavior in spin valves with and without antiferromagnetic subsystems

Citation
Yf. Li et al., Memory effect and temperature behavior in spin valves with and without antiferromagnetic subsystems, J APPL PHYS, 86(10), 1999, pp. 5692-5695
Citations number
23
Categorie Soggetti
Apllied Physucs/Condensed Matter/Materiales Science
Journal title
JOURNAL OF APPLIED PHYSICS
ISSN journal
00218979 → ACNP
Volume
86
Issue
10
Year of publication
1999
Pages
5692 - 5695
Database
ISI
SICI code
0021-8979(19991115)86:10<5692:MEATBI>2.0.ZU;2-B
Abstract
Temperature behavior and memory effect in standard spin valves (SV) and SVs with synthetic antiferromagnetic (Co/Ru/Co) (SV-SAF) subsystems have been studied. SV-SAFs show much better temperature stability. Memory effect refe rs to the phenomenon that the exchange bias can be altered at temperatures (T-R's) much lower than the blocking temperature (T-B), and these temperatu res (T-R's) are imprinted into SVs. The memory effect greatly deteriorates the magnetoresistance behaviors in SV. Our results suggest that the memory effect is caused by a distribution of local blocking temperatures (T-b's). The magnetization state in the pinned layer is critical in determining the temperature behavior of H-E and magnetoresistance. By partially reversing t he magnetization in the pinned ferromagnetic (FM) layers, we are able to se parate the temperature dependencies of the local exchange bias (H-e) associ ated with regions consisting of different T-b's. Two features have been obs erved: (1) the local exchange bias (H-e) with a narrow T-b distribution has a weak temperature dependence; (2) the simple algebraic sum of local H-e's nearly reproduce the total H-E with the difference between these two quant ities representing the domain wall energy in the FM layer. On the other han d, SV-SAFs show strong resistance to memory effects because of two factors; the strong exchange coupling through the Ru layer, and the net magnetic mo ment of Co/Ru/Co layers in SV-SAF being close to zero. The former makes the two SV-SAF FM layers behave coherently, while the latter makes the interac tion between the SV-SAF and the external field negligibly small. (C) 1999 A merican Institute of Physics. [S0021-8979(99)08621-1].