P. Schobinger‐Papamantellos

ETH Zurich

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K.H.J. Buschow

University of Amsterdam

J. Rodrı́guez-Carvajal

Institut Laue-Langevin

K.H.J. Buschow

University of Amsterdam

K.H.J. Buschow

University of Amsterdam

C. Ritter

Institut Laue-Langevin

F.R. de Boer

Charles University

C.H. de Groot

University of Southampton

G. André

CEA Paris-Saclay

Peter Fischer

ETH Zurich

O. Oleksyn

Lviv State University of Internal Affairs

Cooperative Institutions

ETH Zurich

Centre National de la Recherche Scientifique

Paul Scherrer Institute

University of Amsterdam

University of Geneva

Board of the Swiss Federal Institutes of Technology

Institut Laue-Langevin

École Polytechnique Fédérale de Lausanne

Flanders Marine Institute

University of Warwick

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Loss of ferromagnetism in PrYSi3 − δ

Journal of Alloys and Compounds (1992)

P. Schobinger‐Papamantellos K.H.J. Buschow

Substitution (logic)

10.1016/0925-8388(92)90545-k

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Citations (2)

Mictomagnetic behaviour of CeNi0.84Sn2: A neutron diffraction and magnetic study

Physica B Condensed Matter (1997)

P. Schobinger‐Papamantellos J. Rodrı́guez-Carvajal K. Prokes̆K.H.J. Buschow

Orthorhombic crystal system

Magnetic structure

10.1016/s0921-4526(96)01093-9

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Citations (0)

Magnetic ordering of rare earth monochalcogenides. I. Neutron diffraction investigation of CeS, NdS, NdSe, NdTe and TbSe

Journal of Physics C Solid State Physics (1974)

P. Schobinger‐Papamantellos A. Niggli Peter Fischer E. Kaldis V Hildebrandt

The magnetic structures and ordered moments have been determined at 4.2K for the metallic antiferromagnets CeS, NdS, NdSe, NdTe, and TbSe with NaCl structure by means of neutron diffraction. In contrast to the monopnictides, the monochalcogenides of both light and heavy rare earths have FCC type II antiferromagnetic ordering at low temperatures similar to FeO and MnO. Except NdS, where the magnetic moments are tilted by 24 degrees out of the (111) direction, the moments point along the inversion triad which leads to rhombohedral symmetry of the magnetic structure (Shubnikov group R13c). As a consequence of magnetoelastic interactions the FCC lattice of TbSe is rhombohedrally distorted at 4.2K.

Point reflection

Magnetic structure

Lattice (music)

10.1088/0022-3719/7/11/017

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Citations (39)

ChemInform Abstract: Antiferromagnetic Ordering in the Novel Ho3Ge5 and HoGe1.85 Compounds Studied by X-Ray and Neutron Diffraction.

ChemInform (1999)

O. Zaharko P. Schobinger‐Papamantellos C. Ritter

Abstract ChemInform is a weekly Abstracting Service, delivering concise information at a glance that was extracted from about 100 leading journals. To access a ChemInform Abstract of an article which was published elsewhere, please select a “Full Text” option. The original article is trackable via the “References” option.

10.1002/chin.199901002

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Crystallographic and magnetic structure of TbGe2

Journal of the Less Common Metals (1988)

P. Schobinger‐Papamantellos D.B. de Mooij K.H.J. Buschow

Terbium

Orthorhombic crystal system

Magnetic structure

Lattice (music)

Lattice constant

10.1016/0022-5088(88)90140-3

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Citations (22)

A neutron diffraction study of the magnetic ordering of LuMn6Ge6

Journal of Alloys and Compounds (1995)

P. Schobinger‐Papamantellos G. André J. Rodrı́guez-Carvajal J.H.V.J. Brabers K.H.J. Buschow

Magnetic structure

10.1016/0925-8388(95)01630-9

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Citations (22)

Magnetic properties of studied by magnetization and neutron diffraction

Journal of Physics Condensed Matter (1996)

P. Schobinger‐Papamantellos J. Rodrı́guez-Carvajal K. Prokes̆K.H.J. Buschow

The magnetic properties of the compound were studied by magnetization measurements and neutron diffraction. The refinement of the nuclear structure shows that this compound is slightly Ni-deficient, the corresponding formula being . At 1.5 K two coexisting magnetic phases were observed in equal amounts. One of these is ferromagnetic with . The other phase is an antiferromagnetic modulated phase (antiphase domain type with two amplitudes) with . Its magnetic ordering can be described in terms of two propagation vectors ( magnetic lattice) and . The ordered magnetic moment value at 1.5 K in both phases is per Ce atom and points in the same direction along c. Above 2 K the wavevector becomes incommensurate with the crystal lattice. The observation of two magnetic phases is attributed to the occurrence of concentration fluctuations associated with the Ni deficiency.

Magnetic structure

Wave vector

10.1088/0953-8984/8/44/014

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Citations (11)

Magnetic properties and neutron diffraction of TbMn4Al8

Journal of Alloys and Compounds (1996)

P. Schobinger‐Papamantellos Peter Fischer C.H. de Groot F.R. de Boer K.H.J. Buschow

Magnetic structure

10.1016/0925-8388(95)01906-5

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Citations (17)