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通过高分辨率中子光谱研究CoF₂中的反常超精细相互作用。

Anomalous hyperfine interaction in CoF(2) investigated by high resolution neutron spectroscopy.

作者信息

Chatterji Tapan, Schneider G J

机构信息

JCNS, Forschungszentrum Jülich Outstation at Institut Laue-Langevin, BP 156, 38042 Grenoble Cedex 9, France.

出版信息

J Phys Condens Matter. 2009 Oct 28;21(43):436008. doi: 10.1088/0953-8984/21/43/436008. Epub 2009 Oct 8.

Abstract

We investigated the low energy excitations in CoF(2) in the µeV range with a back-scattering neutron spectrometer. The energy scans on a CoF(2) powder sample revealed inelastic peaks at E = 0.728 ± 0.008 µeV at T = 3.46 K on both energy gain and energy loss sides. The inelastic peaks move gradually towards lower energy with increasing temperature and finally merge with the elastic peak at the electronic magnetic ordering temperature T(N)≈37 K. We interpret the inelastic peaks to be due to the transition between the hyperfine-split nuclear level of the (59)Co isotopes with spin I = 7/2. We have shown that the energy of the inelastic peak or the hyperfine splitting in CoF(2) can be treated as an order parameter of the antiferromagnetic phase transition and yields the critical exponent β = 0.313 ± 0.007, consistent with the neutron diffraction results and also the three-dimensional Ising character of the magnetic system. The determined hyperfine splitting in CoF(2) deviates from the linear relationship between the ordered electronic magnetic moment and the hyperfine splitting in Co, Co-P amorphous alloys and CoO, presumably due to the presence of an unquenched orbital moment.

摘要

我们使用背散射中子光谱仪研究了CoF₂在微电子伏特范围内的低能激发。对CoF₂粉末样品的能量扫描显示,在T = 3.46 K时,能量增益和能量损失两侧在E = 0.728±0.008微电子伏特处都出现了非弹性峰。随着温度升高,非弹性峰逐渐向低能量移动,最终在电子磁有序温度T(N)≈37 K时与弹性峰合并。我们将非弹性峰解释为自旋I = 7/2的(59)Co同位素的超精细分裂核能级之间的跃迁所致。我们已经表明,CoF₂中非弹性峰的能量或超精细分裂可以被视为反铁磁相变的序参量,并得出临界指数β = 0.313±0.007,这与中子衍射结果以及磁系统的三维伊辛特性一致。CoF₂中确定的超精细分裂偏离了Co、Co-P非晶合金和CoO中有序电子磁矩与超精细分裂之间的线性关系,这可能是由于存在未淬灭的轨道矩。

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