Journal
JOURNAL OF PHYSICS D-APPLIED PHYSICS
Volume 47, Issue 36, Pages -Publisher
IOP PUBLISHING LTD
DOI: 10.1088/0022-3727/47/36/365003
Keywords
magnetic dynamics; nanoparticles of antiferromagnetic materials; nano-crystallinity
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Funding
- Danish Councils for Independent Research
- National Research Initiative of the US Department of Agriculture Cooperative State Research, Education, and Extension Service [2007-35107-17893]
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Goethite (alpha-FeOOH) is a common nanocrystalline antiferromagnetic mineral. However, it is typically difficult to study the properties of isolated single-crystalline goethite nanoparticles, because goethite has a strong tendency to form particles of aggregated nanograins often with low-angle grain boundaries. This nanocrystallinity leads to complex magnetic properties that are dominated by magnetic fluctuations in interacting grains. Here we present a study of the magnetic properties of 5.7 nm particles of goethite by use of magnetization measurements, inelastic neutron scattering and Mossbauer spectroscopy. The 'ultra-small' size of these particles (i.e. that the particles consist of one or only a few grains) allows for more direct elucidation of the particles' intrinsic magnetic properties. We find from ac and dc magnetization measurements a significant upturn of the magnetization at very low temperatures most likely due to freezing of spins in canted spin structures. From hysteresis curves we estimate the saturation magnetization from uncompensated magnetic moments to be sigma(s) = 0.044 A m(2) kg(-1) at room temperature. Inelastic neutron scattering measurements show a strong signal from excitations of the uniform mode (q = 0 spin waves) at temperatures of 100-250 K and Mossbauer spectroscopy studies show that the magnetic fluctuations are dominated by 'classical' superparamagnetic relaxation at temperatures above similar to 170 K. From the temperature dependence of the hyperfine fields and the excitation energy of the uniform mode we estimate a magnetic anisotropy constant of around 1.0 x 10(5) J m(-3).
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