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EuNiGe 3 , an anisotropic antiferromagnet

Authors :
Arumugam Thamizhavel
Pierre Bonville
S. K. Dhar
Arvind Maurya
Department of Condensed Matter Physics and Materials Science [TIFR] (CMPMS)
Tata Institute for Fundamental Research (TIFR)
Laboratoire Nano-Magnétisme et Oxydes (LNO)
Service de physique de l'état condensé (SPEC - UMR3680)
Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay-Centre National de la Recherche Scientifique (CNRS)-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay-Centre National de la Recherche Scientifique (CNRS)-Institut Rayonnement Matière de Saclay (IRAMIS)
Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay
Source :
Journal of Physics: Condensed Matter, Journal of Physics: Condensed Matter, IOP Publishing, 2014, 26 (21), pp.216001. ⟨10.1088/0953-8984/26/21/216001⟩, Journal of Physics: Condensed Matter, 2014, 26 (21), pp.216001. ⟨10.1088/0953-8984/26/21/216001⟩
Publication Year :
2014
Publisher :
HAL CCSD, 2014.

Abstract

International audience; Single crystals of EuNiGe 3 crystallizing in the non-centrosymmetric BaNiSn 3-type structure have been grown using In flux, enabling us to explore the anisotropic magnetic properties which was not possible with previously reported polycrystalline samples. The EuNiGe 3 single crystalline sample is found to order antiferromagnetically at 13.2 K as revealed from the magnetic susceptibility, heat capacity and electrical resistivity data. The low temperature magnetization M(H) is distinctly different for field parallel to ab-plane and c-axis; the ab-plane magnetization varies nearly linearly with field before the occurrence of an induced ferromagnetic phase (spin-flip) at 6.2 Tesla; on the other hand M(H) along the c-axis is accompanied by two metamagnetic transitions followed by a spin-flip at 4.1 T. A model including anisotropic exchange and dipole-dipole interactions reproduces the main features of magnetization plots but falls short of full representation. (H,T) phase diagrams have been constructed for the field applied along the principal directions. From the 151 Eu Mössbauer spectra, we determine that the 13.2 K transition leads to an incommensu-rate antiferromagnetic intermediate phase followed by a transition near 10.5 K to a commensurate antiferromagnetic configuration.

Details

Language :
English
ISSN :
09538984 and 1361648X
Database :
OpenAIRE
Journal :
Journal of Physics: Condensed Matter, Journal of Physics: Condensed Matter, IOP Publishing, 2014, 26 (21), pp.216001. ⟨10.1088/0953-8984/26/21/216001⟩, Journal of Physics: Condensed Matter, 2014, 26 (21), pp.216001. ⟨10.1088/0953-8984/26/21/216001⟩
Accession number :
edsair.doi.dedup.....4c0936db992085225847064b89265c04