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| Hauptseite > Publikationsdatenbank > Magnetic order of the hexagonal rare-earth manganite Dy(0.5)Y(0.5)MnO(3) > print |
| Hauptseite > Publikationsdatenbank > Magnetic order of the hexagonal rare-earth manganite Dy(0.5)Y(0.5)MnO(3) > print |
| 001 | 20188 | ||
| 005 | 20250129094211.0 | ||
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| 084 | _ | _ | |2 WoS |a Physics, Condensed Matter |
| 100 | 1 | _ | |0 P:(DE-HGF)0 |a Helton, J.S. |b 0 |
| 245 | _ | _ | |a Magnetic order of the hexagonal rare-earth manganite Dy(0.5)Y(0.5)MnO(3) |
| 260 | _ | _ | |a College Park, Md. |b APS |c 2011 |
| 300 | _ | _ | |a 064434 |
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| 440 | _ | 0 | |0 4919 |a Physical Review B |v 84 |x 1098-0121 |y 6 |
| 500 | _ | _ | |a We thank J. W. Lynn for guidance and helpful discussions. J. S. H. acknowledges support from the NRC/NIST Postdoctoral Associateship Program. This work was supported in part by the National Science Foundation under Agreement No. DMR-0944772. |
| 520 | _ | _ | |a Hexagonal Dy0.5Y0.5MnO3, a multiferroic rare-earth manganite with geometrically frustrated antiferromagnetism, has been investigated with single-crystal neutron diffraction measurements. Below 3.4 K magnetic order is observed on both the Mn (antiferromagnetic) and Dy (ferrimagnetic) sublattices that is identical to that of undiluted hexagonal DyMnO3 at low temperature. The Mn moments undergo a spin reorientation transition between 3.4 K and 10 K, with antiferromagnetic order of the Mn sublattice persisting up to 70 K; the antiferromagnetic order in this phase is distinct from that observed in undiluted (h) DyMnO3, yielding a qualitatively new phase diagram not seen in other hexagonal rare-earth manganites. A magnetic field applied parallel to the crystallographic c axis will drive a transition from the antiferromagnetic phase into the low-temperature ferrimagnetic phase with little hysteresis. |
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