Magnetic properties of Co/Pt multilayers deposited on silicon dot arrays

Citation
S. Landis et al., Magnetic properties of Co/Pt multilayers deposited on silicon dot arrays, PHYS REV B, 62(18), 2000, pp. 12271-12281
Citations number
38
Categorie Soggetti
Apllied Physucs/Condensed Matter/Materiales Science
Journal title
PHYSICAL REVIEW B
ISSN journal
01631829 → ACNP
Volume
62
Issue
18
Year of publication
2000
Pages
12271 - 12281
Database
ISI
SICI code
0163-1829(20001101)62:18<12271:MPOCMD>2.0.ZU;2-2
Abstract
Arrays of silicon dots down to 200 nm in size have been prepared by standar d lithography and etching techniques, and then covered by different (Co-0.5 nm/Pt-1.8 nm) multilayers which exhibit perpendicular magnetic anisotropy. On unpatterned substrates, the coercive field varies between 120 and 400 O e, depending on the buffer thickness and on the number of layers. Magnetic force microscopy (MFM) images show magnetic domains about 1.2 mum in size. Deposition of these multilayers on patterned silicon substrates shows that the profile of the magnetic dots is the same as the initial Si dot profile even when the amount of magnetic material represents 60% of the dot height. Atomic force microscopy cross sections indicate that a negligible amount o f material is deposited on the side walls of the dots. MFM images of arrays with a dot spacing large enough to explore the bottom of the grooves show that the magnetic domains in areas between the dots are of the same size as on the unpatterned area, although their coercive field is increased from 1 70 to 300 Oe. On the top of the dots, single-domain configurations are obse rved, and the coercive field of the dots ranges from 1600 to 2400 Oe. This distribution of switching fields, which only weakly depends on the dot size , is mainly related to the detailed shape of the dots (in particular the sh arpness of the corners) and not to their magnetostatic interaction. This co nfers to each individual dot a well-defined coercive field. The magnetizati on reversal of a given dot weakly influences its first neighbors, which mea ns that the dots are essentially independent of each other for the range of Co and Pt thickness used in this study. In the same way, no significant co upling is mediated by the continuous magnetic layer in the bottom of the gr ooves. These results are confirmed by micromagnetic calculations of the mag netic dot-dot and dot-groove interactions for the various geometries that w e have investigated.