Itinerant spin excitations near the hidden order transition in URu2Si2

被引:21
作者
Janik, J. A. [1 ,2 ]
Zhou, H. D. [2 ]
Jo, Y-J [2 ]
Balicas, L. [2 ]
MacDougall, G. J. [3 ]
Luke, G. M. [3 ,4 ]
Garrett, J. D. [5 ]
McClellan, K. J. [6 ]
Bauer, E. D. [6 ]
Sarrao, J. L. [6 ]
Qiu, Y. [7 ,8 ]
Copley, J. R. D. [7 ]
Yamani, Z. [9 ]
Buyers, W. J. L. [4 ,9 ]
Wiebe, C. R. [1 ,2 ]
机构
[1] Florida State Univ, Dept Phys, Tallahassee, FL 32306 USA
[2] Florida State Univ, Natl High Magnet Field Lab, Tallahassee, FL 32306 USA
[3] McMaster Univ, Dept Phys & Astron, Hamilton, ON L8S 4M1, Canada
[4] Canadian Inst Adv Res, Toronto, ON M5G 1Z8, Canada
[5] McMaster Univ, Brockhouse Inst Mat Res, Hamilton, ON L8S 4M1, Canada
[6] Los Alamos Natl Lab, Sci Technol & Engn Directorate, Los Alamos, NM 87545 USA
[7] NIST, Ctr Neutron Res, Gaithersburg, MD 20899 USA
[8] Univ Maryland, Dept Mat Sci & Engn, College Pk, MD 20742 USA
[9] CNBC, Natl Res Council, Chalk River, ON K0J 1J0, Canada
基金
加拿大自然科学与工程研究理事会;
关键词
MAGNETIC EXCITATIONS; NEUTRON-SCATTERING; FERMI-SURFACE; FLUCTUATIONS;
D O I
10.1088/0953-8984/21/19/192202
中图分类号
O469 [凝聚态物理学];
学科分类号
070205 ;
摘要
By means of neutron scattering we show that the high temperature precursor to the hidden order state of the heavy fermion superconductor URu2Si2 exhibits heavily damped incommensurate paramagnons whose strong energy dispersion is very similar to that of the long-lived longitudinal f spin excitations that appear below T-0. This suggests that there is a strongly hybridized character to the itinerant excitations observed previously above the hidden order transition. Here we present evidence that the itinerant excitations, like those in chromium, are due to Fermi surface nesting of hole and electron pockets; hence the hidden order phase probably originates from a Fermi surface instability. We identify wavevectors that span nested regions of a f-d hybridized band calculation and that match the neutron spin crossover from incommensurate to commensurate on approach to the hidden order phase.
引用
收藏
页数:4
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