Magnetic ordering in ternary RMn2Ge2 compounds (R Tb, Ho, Er, Tm, Lu) from neutron diffraction study
Identifieur interne : 002C12 ( Main/Exploration ); précédent : 002C11; suivant : 002C13Magnetic ordering in ternary RMn2Ge2 compounds (R Tb, Ho, Er, Tm, Lu) from neutron diffraction study
Auteurs : Gérard Venturini (physicien) [France] ; B. Malaman [France] ; E. Ressouche [France]Source :
- Journal of Alloys and Compounds [ 0925-8388 ] ; 1996.
Descripteurs français
- Pascal (Inist)
- 7550G, Alliage base erbium, Alliage base holmium, Alliage base lutétium, Alliage base terbium, Alliage base thulium, Alliage ternaire, Composé intermétallique, Diffraction neutron, Etude expérimentale, Ferrimagnétique, Germanium alliage, Lanthanide alliage, Manganèse alliage, Moment magnétique, Propriété magnétique, Structure magnétique.
- Wicri :
- topic : Alliage.
English descriptors
- KwdEn :
- Alloy, Alloys comp, Antiferromagnetic, Antiferromagnetic arrangement, Basal plane, Behaviour, Bragg angles, Cell parameter, Cell parameters, Compound, Curie point, Curie temperature, Earth compounds, Erbium base alloys, Experimental study, Fair agreement, Ferrimagnetic materials, Ferromagnetic, Ferromagnetic planes, Germanium alloys, Good accord, Holmium base alloys, Intermetallic compounds, Leciejewicz, Line intensity, Lutetium base alloys, Magn, Magnetic behaviour, Magnetic moments, Magnetic order, Magnetic properties, Magnetic structure, Magnetic sublattice, Magnetization, Manganese alloys, Neel temperature, Neutron, Neutron diffraction, Neutron diffraction patterns, Neutron diffraction study, Phys, Propagating vector, Rare earth, Rare earth alloys, Rare earth compounds, Refined parameters, Solid solution, Spontaneous magnetization, Structure factors, Sublattice, Szytula, Terbium base alloys, Ternary alloys, Thermal variation, Thulium base alloys, Venturini, Whole series.
- Teeft :
- Alloy, Alloys comp, Antiferromagnetic, Antiferromagnetic arrangement, Basal plane, Behaviour, Bragg angles, Cell parameter, Cell parameters, Compound, Curie point, Curie temperature, Earth compounds, Fair agreement, Ferromagnetic, Ferromagnetic planes, Good accord, Leciejewicz, Line intensity, Magn, Magnetic behaviour, Magnetic order, Magnetic properties, Magnetic structure, Magnetic sublattice, Magnetization, Neel temperature, Neutron, Neutron diffraction, Neutron diffraction patterns, Neutron diffraction study, Phys, Propagating vector, Rare earth, Rare earth compounds, Refined parameters, Solid solution, Spontaneous magnetization, Structure factors, Sublattice, Szytula, Thermal variation, Venturini, Whole series.
Abstract
Abstract: The compounds RMn2Ge2 (R = Tb, Ho, Er, Tm, Lu) have been investigated by neutron diffraction. TbMn2Ge2 is a collinear ferrimagnet with the Mn and Tb moment aligned along the c axis (μTB = 8.81(59) μB: μMn = 2.21(44) μB). HoMn2Ge2 exhibits incommensurale ordering below 2.1 K characterized by two wavevectors at 1.3 K: q1 = (0.1543(4), 0.1543(4), 0) and q2 = (0.210(1), 0.007(1), 0). The Mn sublattice remains antiferromagnetic down to 1.3 K (μMn = 2.38(6) μB). The Er moments order ferromagnetically below 5.5 K in ErMn2Ge2 (μMn = 6.81(31) μB). The moments are perpendicular to the c axis. The Mn sublattice remains antiferromagnetic down to 1.8 K (μMn = 2.34(18) μB). The magnetic structure of TmMn2Ge2 is characterized by the propagation vector (0.0.1/2). the Tm moments lying in the basal plane. The ordering of the Tm moments yields a canting of the Mn moments (τ = 21(3)°); μTm = 6.63(18) μB; μMn = 2.28(27) μB). The antiferromagnetic structure of LuMn2Ge2 has been determined (μMn = 2.32(14) μB). The evolution of the magnetic properties of the heavy rare earth compounds RMn2Ge2 is discussed.
Url:
DOI: 10.1016/0925-8388(96)02272-4
Affiliations:
- France
- Auvergne-Rhône-Alpes, Grand Est, Lorraine (région), Rhône-Alpes
- Grenoble, Nancy, Vandoeuvre les Nancy
- Centre national de la recherche scientifique, Institut Jean Lamour, Université de Lorraine
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Le document en format XML
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<term>Bragg angles</term>
<term>Cell parameter</term>
<term>Cell parameters</term>
<term>Compound</term>
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<term>Curie temperature</term>
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<term>Experimental study</term>
<term>Fair agreement</term>
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<term>Ferromagnetic</term>
<term>Ferromagnetic planes</term>
<term>Germanium alloys</term>
<term>Good accord</term>
<term>Holmium base alloys</term>
<term>Intermetallic compounds</term>
<term>Leciejewicz</term>
<term>Line intensity</term>
<term>Lutetium base alloys</term>
<term>Magn</term>
<term>Magnetic behaviour</term>
<term>Magnetic moments</term>
<term>Magnetic order</term>
<term>Magnetic properties</term>
<term>Magnetic structure</term>
<term>Magnetic sublattice</term>
<term>Magnetization</term>
<term>Manganese alloys</term>
<term>Neel temperature</term>
<term>Neutron</term>
<term>Neutron diffraction</term>
<term>Neutron diffraction patterns</term>
<term>Neutron diffraction study</term>
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<front><div type="abstract" xml:lang="en">Abstract: The compounds RMn2Ge2 (R = Tb, Ho, Er, Tm, Lu) have been investigated by neutron diffraction. TbMn2Ge2 is a collinear ferrimagnet with the Mn and Tb moment aligned along the c axis (μTB = 8.81(59) μB: μMn = 2.21(44) μB). HoMn2Ge2 exhibits incommensurale ordering below 2.1 K characterized by two wavevectors at 1.3 K: q1 = (0.1543(4), 0.1543(4), 0) and q2 = (0.210(1), 0.007(1), 0). The Mn sublattice remains antiferromagnetic down to 1.3 K (μMn = 2.38(6) μB). The Er moments order ferromagnetically below 5.5 K in ErMn2Ge2 (μMn = 6.81(31) μB). The moments are perpendicular to the c axis. The Mn sublattice remains antiferromagnetic down to 1.8 K (μMn = 2.34(18) μB). The magnetic structure of TmMn2Ge2 is characterized by the propagation vector (0.0.1/2). the Tm moments lying in the basal plane. The ordering of the Tm moments yields a canting of the Mn moments (τ = 21(3)°); μTm = 6.63(18) μB; μMn = 2.28(27) μB). The antiferromagnetic structure of LuMn2Ge2 has been determined (μMn = 2.32(14) μB). The evolution of the magnetic properties of the heavy rare earth compounds RMn2Ge2 is discussed.</div>
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