Home > Publications database > Magnetic structures in the magnetic phase diagram of Ho$_2$RhIn$_8$ > print |
001 | 189293 | ||
005 | 20230426083119.0 | ||
024 | 7 | _ | |a 10.1103/PhysRevB.91.144404 |2 doi |
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100 | 1 | _ | |a Cermak, Petr |0 P:(DE-Juel1)159141 |b 0 |e Corresponding Author |u fzj |
245 | _ | _ | |a Magnetic structures in the magnetic phase diagram of Ho$_2$RhIn$_8$ |
260 | _ | _ | |a College Park, Md. |c 2015 |b APS |
336 | 7 | _ | |a article |2 DRIVER |
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520 | _ | _ | |a The magnetic phase diagram of the tetragonal Ho2RhIn8 compound has similar features to many related systems, revealing a zero magnetic field AF1 and a field-induced AF2 phases. Details of the magnetic order in the AF2 phase were not reported yet for any of the related compounds. In addition, only the Ho2RhIn8 phase diagram contains a small region of the incommensurate zero-field AF3 phase. We have performed a number of neutron diffraction experiments on single crystals of Ho2RhIn8 using several diffractometers including experiments in both horizontal and vertical magnetic fields up to 4 T. We present details of the magnetic structures in all magnetic phases of the rich phase diagram of Ho2RhIn8. The Ho magnetic moments point along the tetragonal c axis in every phase. The ground-state AF1 phase is characterized by propagation vector k=(1/2,0,0). The more complex ferrimagnetic AF2 phase is described by four propagation vectors k0=(0,0,0),k1=(1/2,0,0),k2=(0,1/2,1/2),k3=(1/2,1/2,1/2). The magnetic structure in the AF3 phase is incommensurate with kAF3=(0.5,δ,0). Our results are consistent with theoretical calculations based on crystal field theory. |
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700 | 1 | _ | |a Prokeš, Karel |b 1 |
700 | 1 | _ | |a Ouladdiaf, Bachir |b 2 |
700 | 1 | _ | |a Boehm, Martin |b 3 |
700 | 1 | _ | |a Kratochvílová, Marie |b 4 |
700 | 1 | _ | |a Javorský, Pavel |b 5 |
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