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Onset of antifeiromagnetism in heavy-fermion metals

机译:重铁金属中反铁磁性的发作

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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 anti-ferromagnetic 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 CeCu_(6-x)Au_x, 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 (x_c = 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.
机译:反铁磁体有两个主要的理论描述。第一种来自原子物理学,它预测具有不成对电子的原子会产生磁矩。在固体中,附近离子的矩之间的耦合随后在低温下产生反铁磁有序。第二个描述基于电子流体或“费米液体”的物理性质,指出库仑相互作用可通过产生自旋密度波来驱动流体采用更稳定的构型。目前尚不清楚哪种观点在反铁磁转变温度消失的“量子临界点”是合适的。在这里,我们报告了金属CeCu_(6-x)Au_x的中子散射和体磁测量结果,这使我们可以区分这两种模型。我们发现证据表明,在临界金浓度(x_c = 0.1)(对应于零的磁有序温度)下,原子对磁性相关具有局部贡献。这种贡献表明,自旋密度波描述中未预料到的破坏费米液体的自旋局部化转变与反铁磁量子临界点重合。

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