001     281911
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024 7 _ |2 doi
|a 10.1103/PhysRevB.92.115116
024 7 _ |2 ISSN
|a 0163-1829
024 7 _ |2 ISSN
|a 0556-2805
024 7 _ |2 ISSN
|a 1095-3795
024 7 _ |2 ISSN
|a 1098-0121
024 7 _ |2 ISSN
|a 1550-235X
024 7 _ |2 Handle
|a 2128/9873
024 7 _ |2 WOS
|a WOS:000360885100005
037 _ _ |a FZJ-2016-01567
082 _ _ |a 530
100 1 _ |0 P:(DE-HGF)0
|a Niklowitz, P. G.
|b 0
|e Corresponding author
245 _ _ |a Role of commensurate and incommensurate low-energy excitations in the paramagnetic to hidden-order transition of URu$_{2}$Si$_{2}$
260 _ _ |a College Park, Md.
|b APS
|c 2015
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520 _ _ |a We report low-energy inelastic neutron scattering data of the paramagnetic (PM) to hidden-order (HO) phase transition at T0=17.5K in URu2Si2. While confirming previous results for the HO and PM phases, our data reveal a pronounced wave-vector dependence of low-energy excitations across the phase transition. To analyze the energy scans we employ a damped harmonic oscillator model containing a fit parameter 1/Γ which is expected to diverge at a second-order phase transition. Counter to expectations the excitations at Q⃗ 1≈(1.4,0,0) show an abrupt steplike suppression of 1/Γ below T0, whereas excitations at Q⃗ 0=(1,0,0), associated with large-moment antiferromagnetism (LMAF) under pressure, show an enhancement and a pronounced peak of 1/Γ at T0. Therefore, at the critical HO temperature T0, LMAF fluctuations become nearly critical as well. This is the behavior expected of a “supervector” order parameter with nearly degenerate components for the HO and LMAF leading to nearly isotropic fluctuations in the combined order-parameter space.
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542 _ _ |i 2015-09-08
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|v 92
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773 _ _ |a 10.1103/PhysRevB.92.115116
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