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Perpendicular Magnetoresistance of Microstructured Pillars in Fe/Cr Magnetic Multilayers

Published online by Cambridge University Press:  03 September 2012

M.A.M. Gijs
Affiliation:
Philips Research Laboratories, 5600 JA Eindhoven, The Netherlands
S.K.J. Lenczowski
Affiliation:
Eindhoven University of Technology, Department of Physics, 5600 MB Eindhoven, The Netherlands
J.B. Giesbers
Affiliation:
Philips Research Laboratories, 5600 JA Eindhoven, The Netherlands
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Abstract

We have fabricated pillar-like microstructures of high vacuum sputtered Fe/Cr Magnetic Multilayers and measured the giant magnetoresistance effect in the configuration where the measuring current is perpendicular to the film plane from 4.2 K to 300 K. At 4.2 K we find a magnetoresistance of 108 % for multilayers with a Fe thickness of 3 nm and a Cr thickness of 1 nm. The pronounced temperature dependence of the perpendicular magnetoresistance is studied for samples with different Cr thicknesses and tentatively explained by electron-Magnon scattering. The low-temperature data are compared with existing low-temperáture models.

Type
Research Article
Copyright
Copyright © Materials Research Society 1993

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References

REFERENCES

[1] Baibich, M.N., Broto, J.M., Fert, A., Nguyen van Dau, F., Petroff, F., Etienne, P., Creuzet, G., Friederich, A., and Chazelas, J., Phys. Rev. Lett. 61, 2427 (1988).Google Scholar
[2] Binasch, G., Grünberg, P., Saurenbach, F., and Zinn, W. Phys. Rev. B 39, 4824, (1989).Google Scholar
[3] Parkin, S.S.P., Bhadra, R., and Roche, K.P., Phys. Rev. Lett. 66, 2152 (1991).Google Scholar
[4] Zhang, S., and Levy, P.M., J. Appl. Phys. 69, 4786 (1991).Google Scholar
[5] Johnson, M., Phys. Rev. Lett. 67, 3594 (1991).Google Scholar
[6] Bauer, G.E.W., Phys. Rev. Lett. 69, 1676 (1992).Google Scholar
[7] Lee, S.-F., Pratt, W.P. Jr, Yang, Q., Holody, P., Loloee, R., Schroeder, P.A., and Bass, J., J. Magn. Magn. Mat. 118, L1 (1993).Google Scholar
[8] Camblong, H.E., Zhang, S., and Levy, P.M., Phys. Rev. B 47, 4735 (1993).Google Scholar
[9] Valet, T., and Fert, A., submitted to Phys. Rev. B.Google Scholar
[10] Pratt, W.P. Jr, Lee, S.-F., Slaughter, J.M., Loloee, R., Schroeder, P.A., and Bass, J., Phys. Rev. Lett. 66, 3060 (1991);Google Scholar
Lee, S.-F., Pratt, W.P. Jr, Loloee, R., Schroeder, P.A., and Bass, J., Phys. Rev. B 46, 548 (1992);Google Scholar
Schroeder, P.A., Bass, J., Holody, P., Lee, S.-F., Loloee, R. Pratt, W.P. Jr, and Yang, Q., to be published.Google Scholar
[11] Schroeder, P., private communication.Google Scholar
[12] Gijs, M.A.M., and Okada, M., Phys. Rev. B 46, 2908 (1992);Google Scholar
Gijs, M.A.M., and Okada, M., J. Magn. Magn. Mat. 113, 105 (1992).Google Scholar
[13] Gijs, M.A.M., Lenczowski, S.K.J., and Giesbers, J.B., Phys. Rev. Lett., to be published.Google Scholar
[14] Parkin, S.S.P., More, N., and Roche, K.P., Phys. Rev. Lett. 64, 2304 (1990).Google Scholar
[15] We define the MR as (R Max R sat ) / R sat , where R Max is the maximum resistance at zero field and R sat the resistance value at saturation of the giant MR effect.Google Scholar
[16] Mills, D.L., Fert, A., and Campbell, I.A., Phys. Rev. B 4, 196 (1971).Google Scholar
[17] Mattson, J.E., Brubaker, M.E., Sowers, C.H., Conover, M., Qiu, Z., and Bader, S.D., Phys. Rev. B 44, 9378 (1991).Google Scholar
[18] Gijs, M.A.M., Giesbers, J. B., Lenczowski, S.K.J., and Janssen, H.H.J.M., Appl. Phys. Lett., to be published.Google Scholar
[19] Bauer, G.E.W., Gijs, M.A.M., Lenczowski, S.K.J., and Giesbers, J.B., J. Magn. Magn. Mat., to be published.Google Scholar
[20] Büttiker, M., IBM J. Res. Dev. 32, 317 (1988).Google Scholar