We report measurements of the magnetoresistivity of CuMn 4.7% and CuMn 1.35% after a number of different magnetic and thermal cycles in the spin glass state. First, our CuMn 4.7% sample was cooled in zero field down to 1.2 K and then submitted for a short time to some maximum field Hmax. Immediately after Hmax was removed the low field (LF) Δρ versus H curve was plotted. Similar low H measurements were then repeated for increasing strengths of Hmax. Two marked shoulders take place at Hmax≊15 kG and become very sharp for Hmax≳30 kG. In order to see whether or not the LF loop is reproducible we measured the same loop about 10 times and found a marked narrowing of the cycle of about 40%. This result cannot be described by a rigid anisotropy axis for which we rather expect a widening of the loop. Examples showing how the form of the LF magnetoresistance loop changes when the temperature is varied in H=0 are presented.
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1 November 1982
Research Article|
November 01 1982
Effect of thermal and field cycling on the magnetoresistivity of CuMn spin glass
S. Senoussi
S. Senoussi
Laboratoire de Physique des Solides, Université Paris‐Sud, Bât. 510, 91405 Orsay Cédex, France
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J. Appl. Phys. 53, 8234–8236 (1982)
Citation
S. Senoussi; Effect of thermal and field cycling on the magnetoresistivity of CuMn spin glass. J. Appl. Phys. 1 November 1982; 53 (11): 8234–8236. https://doi.org/10.1063/1.330336
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