TY - JOUR
T1 - Microscopic mechanisms of giant magnetoresistance
AU - Vouille, C.
AU - Barthélémy, A.
AU - Mpondo, F. Elokan
AU - Fert, A.
AU - Schroeder, P. A.
AU - Hsu, Shih-ying
AU - Reilly, A.
AU - Loloee, R.
PY - 1999/1/1
Y1 - 1999/1/1
N2 - We present magnetoresistance measurements aimed at answering several open questions in the understanding of giant magnetoresistance (GMR). Our measurements are performed on (F1/N/F2/N) multilayers in which N is a nonmagnetic metal (Cu or Cr), and F1 and F2 are various ferromagnetic metals or alloys. In current perpendicular to the plane (CPP) measurements on (F1/Cu/Co/Cu) multilayers, where F1 is Fe, Co, or Ni doped with impurities, we observe an inversion of the GMR for V or Cr impurities; this demonstrates, first the importance of the extrinsic effects in GMR and secondly the possibility of obtaining negative as well as positive values of the bulk spin asymmetry coefficient β. A compensation thickness with zero GMR is found when the bulk and interface spin asymmetry have opposite signs in the same layer. We interpret the sign of β in models of electronic structure. Measurements on other series of multilayers allow us to show that the interface spin asymmetry coefficient ? can also be positive (interfaces with Cu) or negative (interfaces with Cr). Finally, the comparison between CPP and CIP data obtained on the same samples sheds light on the different role of the interface intrinsic potential in the two geometries.
AB - We present magnetoresistance measurements aimed at answering several open questions in the understanding of giant magnetoresistance (GMR). Our measurements are performed on (F1/N/F2/N) multilayers in which N is a nonmagnetic metal (Cu or Cr), and F1 and F2 are various ferromagnetic metals or alloys. In current perpendicular to the plane (CPP) measurements on (F1/Cu/Co/Cu) multilayers, where F1 is Fe, Co, or Ni doped with impurities, we observe an inversion of the GMR for V or Cr impurities; this demonstrates, first the importance of the extrinsic effects in GMR and secondly the possibility of obtaining negative as well as positive values of the bulk spin asymmetry coefficient β. A compensation thickness with zero GMR is found when the bulk and interface spin asymmetry have opposite signs in the same layer. We interpret the sign of β in models of electronic structure. Measurements on other series of multilayers allow us to show that the interface spin asymmetry coefficient ? can also be positive (interfaces with Cu) or negative (interfaces with Cr). Finally, the comparison between CPP and CIP data obtained on the same samples sheds light on the different role of the interface intrinsic potential in the two geometries.
UR - http://www.scopus.com/inward/record.url?scp=0000756896&partnerID=8YFLogxK
U2 - 10.1103/PhysRevB.60.6710
DO - 10.1103/PhysRevB.60.6710
M3 - Article
AN - SCOPUS:0000756896
SN - 1098-0121
VL - 60
SP - 6710
EP - 6722
JO - Physical Review B - Condensed Matter and Materials Physics
JF - Physical Review B - Condensed Matter and Materials Physics
IS - 9
ER -