Hostname: page-component-76fb5796d-25wd4 Total loading time: 0 Render date: 2024-04-30T02:47:23.962Z Has data issue: false hasContentIssue false

Ion Beam Deposited Gmr Materials

Published online by Cambridge University Press:  17 March 2011

J. M. Lannon Jr.
Affiliation:
MCNC, Materials and Electronic Technologies Division, Research Triangle Park, NC, lannon@mcnc.org
C.C. Pace
Affiliation:
MCNC, Materials and Electronic Technologies Division, Research Triangle Park, NC
D. Temple
Affiliation:
MCNC, Materials and Electronic Technologies Division, Research Triangle Park, NC
G.E McGuire
Affiliation:
MCNC, Materials and Electronic Technologies Division, Research Triangle Park, NC
A.F. Hebard
Affiliation:
Department of Physics, University of Florida, Gainesville, FL
M. Ray
Affiliation:
Integrated Electro-Optics, Inc., Raleigh, NC
Get access

Abstract

Ion beam sputter deposition (IBSD) techniques for deposition of giant magnetoresistance (GMR) films have been studied using an automated IBSD system designed and built in-house. We have studied the properties of Fe/Cr multilayers deposited using either Ar or Xe ions with the primary ion beam energy varying from 500 eV to 1100 eV. The films were characterized using transmission electron microscopy (TEM), atomic force microscopy (AFM), Auger electron spectroscopy (AES), X-ray photoelectron spectroscopy (XPS), secondary ion mass spectroscopy (SIMS), magnetization measurements, and magnetoresistance measurements. The maximum value of GMR obtained was 49% (measured at 10K). For the Cr spacer thickness layer chosen, this GMR ratio is larger than the values reported for polycrystalline Fe/Cr multilayers deposited by magnetron sputtering. In general, we have found that GMR ratios for the Fe/Cr multilayers increase with decreasing primary ion beam energy, and are greater for films deposited using Xe ions than for films deposited using Ar ions. We explain the observed effects on the basis of energy distributions of sputtered atoms and backscattered working gas atoms (neutrals). The energy distributions were calculated using TRIM (Transport of Ions in Matter) software based on the Monte Carlo method.

Type
Research Article
Copyright
Copyright © Materials Research Society 2002

Access options

Get access to the full version of this content by using one of the access options below. (Log in options will check for institutional or personal access. Content may require purchase if you do not have access.)

References

REFERENCES

1. Baibich, M.N., Broto, J.M., Fert, A., Dau, F. Nguyen Van, Petroff, F., Etienne, P., Creuzet, G., Friedrich, A., and Chazelas, J., Phys. Rev. Lett. 61, 2472 (1988).Google Scholar
2. Berg, H.A.M. van den, in Magnetic Multilayers and Giant Magnetoresistance: Fundamentals and Industrial Applications, edited by Hartmann, U. (Springer-Verlag, Berlin Heidelberg, 2000), p. 179.Google Scholar
3. Parkin, S.S.P., in Ultrathin Magnetic Structures II, edited by Heinrich, B. and Bland, J.A.C. (Springer-Verlag, Berlin Heidelberg, 1994) p. 148.Google Scholar
4. Gurney, B.A., Baumgart, P., Wilhoit, D.R., Dieny, B., and Speriosu, V.S., J. Appl. Phys. 70, 5867 (1991).Google Scholar
5. Marrows, C.H., Hickey, B.J., Malinowska, M., and Meny, C., IEEE Transactions on Magnetics 33 (5), 3673 (1997).Google Scholar
6. Ziegler, J., Biersack, J., and Littmark, U., The Stopping and Range of Ions in Solids, vol 1 of The Stopping and Range of Ions in Matter (Pergamon, Oxford, 1985).Google Scholar
7. Seitz, F., Discoveries of the Faraday Society 5, 271 (1947).Google Scholar
8. Fullerton, E.E., Conover, M.J., Mattson, J.E., Sowers, C.H., and Bader, S.D., Phys. Rev. B 48 (21), 15755 (1993).Google Scholar
9. TRIM code (now called SRIM) is shareware that can be downloaded from www.srim.org.Google Scholar