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Giant magnetoresistance of magnetic multilayer point contacts
Author(s) -
K. P. Wellock,
S.J.C.H. Theeuwen,
J. Caro,
N. N. Gribov,
R. P. van Gorkom,
S. Radelaar,
F.D. Tichelaar,
B. J. Hickey,
C. H. Marrows
Publication year - 1999
Publication title -
physical review. b, condensed matter
Language(s) - English
Resource type - Journals
eISSN - 1095-3795
pISSN - 0163-1829
DOI - 10.1103/physrevb.60.10291
Subject(s) - giant magnetoresistance , materials science , etching (microfabrication) , magnetoresistance , layer (electronics) , electrode , molecular beam epitaxy , transmission electron microscopy , condensed matter physics , optoelectronics , sputtering , thin film , epitaxy , magnetic field , composite material , nanotechnology , chemistry , physics , quantum mechanics
of the multilayer electrode. When corrected for this, the maximum point-contact GMR was 3%. The multilayer structure at some depth in the constriction was disrupted, as observed by transmission electron microscopy. This was identified as a cause of the low GMR, together with contamination and an oxide layer in the constriction, resulting from ex situ sample rotation. The second generation was fabricated by sputtering of a coupled Co/Cu multilayer before etching of the nanohole, giving a proper multilayer at the constriction. Further, the GMR signal from the electrode was shorted by a thick Cu cap. This did not bring the expected increase of the GMR (ratio<5%), indicating that the so-called dead layers and the quality of the interface between the GMR system and the contacting metal were limiting. This interface quality was strongly improved for the third generation of contacts by using in situ rotation, while the question of multilayer quality was avoided by shifting to granular Co/Au. Granular Co/Au in the constriction was obtained by growing a discon- tinuous Co layer by MBE. The maximum GMR ratio of the granular contacts was 14%, an improvement of a factor 3. These contacts displayed small jumps in the GMR, two-level fluctuations in the resistance time trace and ballistic transport, the latter being evident from phonon peaks in the point-contact spectrum of a high resistance contact. @S0163-1829~99!01537-4#

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