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Title: Magnetic ordering in Eu2In and Eu2Sn

Journal Article · · Journal of Alloys and Compounds
 [1];  [2];  [3];  [4];  [5];  [5];  [5];  [5];  [5];  [3]
  1. Inst. Laue-Langevin (ILL), Grenoble (France)
  2. McGill Univ., Montreal, QC (Canada)
  3. Univ. of Genova (Italy); Ames Lab., and Iowa State Univ., Ames, IA (United States); National Research Council (CNR), Genova (Italy). Inst. for Superconductors, Innovative Materials and Devices (CNR-SPIN)
  4. Iowa State Univ., Ames, IA (United States)
  5. Ames Lab., and Iowa State Univ., Ames, IA (United States)

Eu2In and Eu2Sn crystallize in the orthorhombic Co2Si-type structure (oP12, Pnma, No. 62) with In and Sn atoms occupying one 4c site and the Eu atoms filling two other 4c sites. Eu2In has a nearly ideal first-order magnetostructural transition (FOMT) at 55 K with a hysteresis of less than 0.1 K, a large entropy change and an adiabatic temperature change of 5.0 K in a field of 2 T. The anhysteretic nature of the FOMT is likely due to there being no change in cell symmetry and relatively small changes in the lattice parameters. There is no magnetostructural transition in Eu2Sn. In this work we present the results of powder neutron diffraction, magnetization, and Eu Mössbauer spectroscopy aimed to investigate the nature of magnetic order for both Eu2In and Eu2Sn. The Eu Mössbauer spectrum of Eu2In at 5 K shows two equal area components, consistent with Eu occupying two equal multiplicity crystallographic sites. However, the different hyperfine fields (B) of 27 T and 17 T suggest that the magnetic environments of the Eu moments on the two 4c sites are different. Neutron diffraction data at 2.5 K show that in Eu2In the order is ferromagnetic, with Eu moments on both Eu sites oriented parallel to the a-axis; moment values of 6.8 μB and 6.5 μB were found. For Eu2Sn measurements find two antiferromagnetic transitions, which are corroborated by neutron diffraction. Analysis of density-functional theory calculations shows negligible energy difference between differing magnetic configurations, indirectly supporting stability of multiple magnetic structures observed experimentally. While the transition at TN1 = 30 K corresponds to the formation of a simple k1 = 0 antiferromagnetic structure with Eu-moments pointing along the b-axis, at TN2 = 13 K a coexisting second magnetic order with k2 = [0, ½, ½] appears.

Research Organization:
Ames Laboratory (AMES), Ames, IA (United States)
Sponsoring Organization:
USDOE Office of Science (SC), Basic Energy Sciences (BES). Materials Sciences & Engineering Division (MSE)
Grant/Contract Number:
AC02-07CH11358
OSTI ID:
2282318
Report Number(s):
IS-J-11,246
Journal Information:
Journal of Alloys and Compounds, Vol. 980; ISSN 0925-8388
Publisher:
ElsevierCopyright Statement
Country of Publication:
United States
Language:
English

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