journal article·2017-02

Magnetic phase diagram of Y 1−x Tb x Mn 6 Sn 6 compounds

A.A. Bykov, Yu.O. Chetverikov, E.V. Moskvin, A.N. Pirogov, S.V. Grigoriev

Publisher page

Abstract

Abstract The Y 1−x Tb x Mn 6 Sn 6 compounds ( x =0, 0.175, 0.2, 0.225, 0.25) were studied by small angle neutron scattering (SANS) and paramagnetic neutron spin echo. The YMn 6 Sn 6 compound is found to be a helimagnet in the whole temperature range below T N =310 K. Close to T N an additional peak of a Lorenz shape was observed at Q =0. The peak is thought to have originated from the ferromagnetic fluctuations of the magnetic Mn moment in the ab-plane of the hexagonal crystal structure. Compounds, in which Y is replaced by Tb, change their magnetic order with the increase of temperature: from easy cone ferromagnetic phase at low T through the helicoidal phase to the ferromagnetic fluctuation close to T N . Temperature-concentration phase diagram of Y 1−x Tb x Mn 6 Sn 6 is built on the basis of the obtained data.
Source: openaire · Quality: candidate unverified · Source record ↗

Research context

OpenAlex topics: Rare-earth and actinide compounds · Magnetic Properties of Alloys · Thermodynamic and Structural Properties of Metals and Alloys

SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.

References (7)

Show source-provided references
1. Venturini · J. Alloy. Compd. · 1996 · 236 · 10210.1016/0925-8388(95)01998-7 ↗
2. Canepa · J. Alloy. Compd. · 2004 · 383 · 1010.1016/j.jallcom.2004.04.024 ↗
3. Zajkov · J. Alloy. Compd. · 2004 · 363 · 4010.1016/S0925-8388(03)00469-9 ↗
4. Bogdanov · Phys. Met. Metallogr. · 2013 · 114 · 56610.1134/S0031918X13070028 ↗
5. Bykov · JETP Lett. · 2015 · 101 · 69910.1134/S0021364015100057 ↗
6. Shigeno · JMMM · 2001 · 226 · 115310.1016/S0304-8853(00)01307-X ↗
7. Rosenfeld · Physica B · 2008 · 403 · 189810.1016/j.physb.2007.10.220 ↗