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Onset of antiferromagnetism in heavy-fermion metals
There are two main theoretical descriptions of antiferromagnets. The first arises from atomic physics, which predicts that atoms with unpaired electrons develop magnetic moments. In a solid, the coupling between moments on nearby ions then yields antiferromagnetic order at low temperatures. The seco...
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Published in: | Nature (London) 2000-09, Vol.407 (6802), p.351-355 |
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Main Authors: | , , , , , , , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | There are two main theoretical descriptions of antiferromagnets. The first
arises from atomic physics, which predicts that atoms with unpaired electrons
develop magnetic moments. In a solid, the coupling between moments on nearby
ions then yields antiferromagnetic order at low temperatures.
The second description, based on the physics of electron fluids or 'Fermi
liquids', states that Coulomb interactions can drive the fluid to adopt
a more stable configuration by developing a spin density wave.
It is at present unknown which view is appropriate at a 'quantum critical
point', where the antiferromagnetic transition temperature vanishes. Here we report neutron scattering and bulk magnetometry
measurements of the metal CeCu6-xAux,
which allow us to discriminate between the two models. We find evidence for
an atomically local contribution to the magnetic correlations which develops
at the critical gold concentration (xc = 0.1
), corresponding to a magnetic ordering temperature of zero. This contribution
implies that a Fermi-liquid-destroying spin-localizing transition, unanticipated
from the spin density wave description, coincides with the antiferromagnetic
quantum critical point. |
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ISSN: | 0028-0836 1476-4687 |
DOI: | 10.1038/35030039 |