Please use this identifier to cite or link to this item: http://www.repositorio.cdtn.br:8080/jspui/handle/123456789/477
Title: Magnetoresistance of mechanically stable Co nanoconstrictions
Title of periodic: Physical Review B New York
metadata.dc.title.subtitlejournal: Condensed Matter and Materials Physics
Authors: Montero, M.I.
Dumas, University of California San Diego, La Jolla, CA, USA)
Liu, G.
Viret, M.
Stoll, O.M
Macedo, Waldemar Augusto de Almeida
Schuller, Ivan K.
Affiliation: University of California San Diego, La Jolla, CA, USA
University of California San Diego, La Jolla, CA, USA
University of California San Diego, La Jolla, CA, USA
University of California San Diego, La Jolla, CA, USA
University of California San Diego, La Jolla, CA, USA; Centro de Desenvolvimento da Tecnologia Nuclear/CDTN, Belo Horizonte, MG, Brasil
University of California San Diego, La Jolla, CS, USA
Issue Date: 2004
Keywords: Cobalt;nanostructures;magnetoresistance;electric resistance
Abstract: We have studied the resistivity and magnetoresistance of mechanically stable Co contacts of nanometer sizes made by electron (e)-beam lithography on Si, GaAs, and Al2O3 substrates. These constrictions were generated using two techniques. The first one uses conventional e-beam lithography to design fingers at different distances touching a perpendicular electrode. These contacts are generally in the tens of nanometers range with resistances as high as 500 V. After ion milling these contacts, resistances as high as 20 kV may be obtained. The second technique consists of Co deposition through a 400 nm hole made in a bilayer resist. The resistance in the current perpendicular to the plane" geometry is monitored during deposition which is stopped when the desired resistance is obtained. Magnetoresistance was measured in a wide range of applied magnetic fields and temperatures. Due to the large shape anisotropy difference between the electrodes, two well-defined coercive fields induce clear switching in the magnetization observable in the resistance. The magnetoresistances are in all cases below 1
and of varying signs. These effects are well within the range of the expected anisotropic magnetoresistance generated at the contacts or their vicinity.
Access: L
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