Abstract: Measurements of the magnetization and specific heat on nanocrystalline TbAl2, TbCu2 and GdAl2 with mean particle diameters below 40 nm show a different behavior from those made on bulk alloys. A reduction of the saturation magnetization quantified in TbAl2 from 8.4 µB/mol for the bulk to 5.8 µB/mol for a 14 nm alloy is attributed to a spin disordered layer on the particle surface. In the specific heat, the lambda anomaly associated to the ferro (?c= 6.6 J/molK, 9.8 J/molK) and to the antiferromagnetic transitions (7.1 J/molK) in the bulk samples, respectively, is smeared out due to finite size effects

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