APS March Meeting 2015
Volume 60, Number 1
Monday–Friday, March 2–6, 2015;
San Antonio, Texas
Session B30: Focus Session: Nanomagnetic Devices II
11:15 AM–2:15 PM,
Monday, March 2, 2015
Room: 206B
Sponsoring
Units:
GMAG DMP
Chair: Kai Liu, University of California, Davis
Abstract ID: BAPS.2015.MAR.B30.4
Abstract: B30.00004 : (001) Oriented $L1_{0}$ FeCuPt for Heat-Assisted Magnetic Recording*
11:51 AM–12:27 PM
Preview Abstract
Abstract
Author:
Kai Liu
(University of California - Davis)
High magnetic anisotropy materials are critical to key technologies such as
ultrahigh density magnetic recording and permanent magnets. Among them,
ordered FePt alloys in the $L$1$_{0}$ phase are particularly sought after, for
the emerging heat-assisted magnetic recording (HAMR) media. However, the
highly desirable properties are associated with the tetragonal $L$1$_{0}$
phase. Key challenges exist in the high annealing temperature necessary to
transform the as-deposited disordered cubic $A$1 phase into the ordered
tetragonal$ L$1$_{0}$ phase and the ability to maintain the magnetic easy axis
perpendicular to the film. We have achieved (001) oriented $L$1$_{0}$ FeCuPt thin films, with magnetic anisotropy up to 3.6 x 10$^{7}$ erg/cm$^{3}$, using atomic-scale multilayer sputtering and rapid thermal
annealing (RTA) at 400 $^{\circ}$C for 10 seconds, which is much more benign
compared to earlier studies [1]. The artificial ordering in the multilayer
structure and a significant tensile stress exerted by the underlying
Si/SiO$_{2}$ during RTA facilitate the formation of (001) oriented
$L$1$_{0}$ phase. The $A$1 to $ L$1$_{0}$ phase transformation has been investigated
by x-ray diffraction and the first-order reversal curve (FORC) method [2]. The
$L$1$_{0}$ ordering takes place via a nucleation-and-growth mode. Traditional
x-ray diffraction is not always reliable in generating a true order
parameter, due to non-ideal crystallinity of the $A$1 phase in some of the
samples. A magnetization-based $L$1$_{0}$ phase fraction is extracted,
providing a quantitative measure of the $L$1$_{0}$ phase homogeneity [3].
\\[4pt]
[1] D. A. Gilbert, L. W. Wang, T. J. Klemmer, J. U. Thiele, C. H. Lai, and
K. Liu, \textit{Appl. Phys. Lett.}, \textbf{102}, 132406, (2013).\\[0pt]
[2] D. A. Gilbert, G. T. Zimanyi, R. K. Dumas, M. Winklhofer, A. Gomez, N.
Eibagi, J. L. Vicent, and K. Liu, \textit{Sci. Rep}, \textbf{4}, 4204 (2014).\\[0pt]
[3] D. A. Gilbert, J. W. Liao, L. W. Wang, J. W. Lau, T. J. Klemmer, J. U.
Thiele, C. H. Lai, and K. Liu, \textit{APL Mater}, \textbf{2}, 086106 (2014).
*This work has been done in collaboration with D. A. Gilbert, J. W. Liao, L. W. Wang, J. W. Lau, T. J Klemmer, J. U. Thiele, and C. H. Lai, supported by the NSF (DMR-1008791).
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2015.MAR.B30.4