Structural, electronic, and magnetic characteristics of Np2Co17

I. Halevy, A. Hen, I. Orion, E. Colineau, R. Eloirdi, J.-C. Griveau, P. Gaczyński, F. Wilhelm, A. Rogalev, J.-P. Sanchez, M. L. Winterrose, N. Magnani, A. B. Shick, and R. Caciuffo
Phys. Rev. B 85, 014434 – Published 30 January 2012

Abstract

A previously unknown neptunium-transition-metal binary compound Np2Co17 has been synthesized and characterized by means of powder x-ray diffraction, 237Np Mössbauer spectroscopy, superconducting-quantum-interference-device magnetometry, and x-ray magnetic circular dichroism (XMCD). The compound crystallizes in a Th2Ni17-type hexagonal structure with room-temperature lattice parameters a=8.3107(1) Å and c=8.1058(1) Å. Magnetization curves indicate the occurrence of ferromagnetic order below TC>350 K. Mössbauer spectra suggest a Np3+ oxidation state and give an ordered moment of μNp=1.57(4) μB and μNp=1.63(4) μB for the Np atoms located, respectively, at the 2b and 2d crystallographic positions of the P63/mmc space group. Combining these values with a sum-rule analysis of the XMCD spectra measured at the neptunium M4,5 absorption edges, one obtains the spin and orbital contributions to the site-averaged Np moment [μS=1.88(9) μB, μL=3.48(9) μB]. The ratio between the expectation value of the magnetic-dipole moment and the spin magnetic moment (mmd/μS=+1.36) is positive as predicted for localized 5f electrons and lies between the values calculated in intermediate-coupling (IC) and jj approximations. The expectation value of the angular part of the spin-orbit-interaction operator is in excellent agreement with the IC estimate. The ordered moment averaged over the four inequivalent Co sites, as obtained from the saturation value of the magnetization, is μCo1.6 μB. The experimental results are discussed against the predictions of first-principles electronic-structure calculations based on the spin-polarized local-spin-density approximation plus the Hubbard interaction.

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  • Received 30 November 2011

DOI:https://doi.org/10.1103/PhysRevB.85.014434

©2012 American Physical Society

Authors & Affiliations

I. Halevy1,2,3, A. Hen2,4, I. Orion2, E. Colineau4, R. Eloirdi4, J.-C. Griveau4, P. Gaczyński4, F. Wilhelm5, A. Rogalev5, J.-P. Sanchez6, M. L. Winterrose3, N. Magnani7, A. B. Shick4,8, and R. Caciuffo4

  • 1Physics Department, Nuclear Research Center Negev, P.O. Box 9001, IL84190 Beer-Sheva, Israel
  • 2Nuclear Engineering Department, Ben Gurion University, IL84105 Beer-Sheva, Israel
  • 3California Institute of Technology, W. M. Keck Laboratory 138-78, Pasadena, California 91125, USA
  • 4European Commission, Joint Research Centre, Institute for Transuranium Elements, Postfach 2340, DE-76125 Karlsruhe, Germany
  • 5European Synchrotron Radiation Facility (ESRF), Boîte Postale 220, FR-38043 Grenoble, France
  • 6SPSMS, UMR-E CEA/UJF-Grenoble 1, INAC, FR-38054 Grenoble, France
  • 7Lawrence Berkeley National Laboratory, Chemical Sciences Division, 1 Cyclotron Road, Berkeley, California 94720, USA
  • 8Institute of Physics, Academy of Sciences of the Czech Republic, Na Slovance 2, CZ-182 21 Prague, Czech Republic

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Vol. 85, Iss. 1 — 1 January 2012

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