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Phys. Rev. Lett. 65, 1643–1646 (1990)

[Issue 13 – 24 September 1990 ]

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Electrical conductivity of magnetic multilayered structures

Peter M. Levy and Shufeng Zhang
Department of Physics, New York University, 4 Washington Place, New York, New York 10003
Albert Fert
Laboratoire de Physique des Solides, Université de Paris(enSud, Bâtiment 510, 91405 Orsay, France
Received 14 March 1990

The electrical-transport properties of magnetic multilayered structures are dominated by three ingredients: (1) the scattering within layers that changes from one layer to another, (2) the additional scattering resistivity due to the roughness of the interfaces between layers, and (3) the resistivity that depends on the orientation of the magnetization of the magnetic layers. In the quasiclassical approach the boundary scattering is treated differently from other sources. Here we present a unified treatment of all sources of resistivity, and determine the origin of the giant magnetoresistance observed in Fe/Cr superlattices.

©1990 The American Physical Society

URL: http://link.aps.org/abstract/PRL/v65/p1643
DOI: 10.1103/PhysRevLett.65.1643
PACS: 72.10.Fk, 72.15.Gd, 75.50.Rr


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References

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  1. M. N. Baibich, J. M. Broto, A. Fert, F. Nguyen Van Dau, F. Petroff, P. Etienne, G. Creuzet, A. Friederich and J. Chazelas, Phys. Rev. Lett. 61, 2472 (1988); A. Barthélémy, A. Fert, M. N. Baibich, S. Hadjoudj, F. Petroff, P. Etienne, R. Cabanel, S. Lequien and G. Creuzet, J. Appl. Phys. 67, 5908 (1990) [dot SPIN][dot INSPEC].
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  8. Z. T e breve_sanovic-acute, M. V. Jaric and S. Maekawa, Phys. Rev. Lett. 57, 2760 (1986); for a treatment of surface-roughness scattering, see also G. Fishman and D. Calecki, Phys. Rev. Lett. 62, 1302 (1989).
  9. G. D. Mahan, Many-Particle Physics (Plenum, New York, 1981), see pp. 591–611; S. Doniach and E. H. Sondheimer, Green's Functions for Solid State Physicists (Benjamin, Reading, MA, 1974), see pp. 92–93, and Chap. 5.
  10. A. Fert and I. A. Campbell, J. Phys. F 6, 849 (1976); I. A. Campbell and A. Fert, in Ferromagnetic Materials, edited by E. P. Wohlfarth (North-Holland, Amsterdam, 1982), Vol. 3, p. 769.
  11. The low-temperature resistivity of the superlattices studied in Ref. 1 are scattered around 60 µ Omega cm; however, for some samples [F. Petroff and A. Fert (private communication)] it can be as large as 80 µ Omega cm or more.


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