Literature DB >> 25001885

Long-range magnetic order in the 5d(2) double perovskite Ba2CaOsO6: comparison with spin-disordered Ba2YReO6.

C M Thompson1, J P Carlo, R Flacau, T Aharen, I A Leahy, J R Pollichemi, T J S Munsie, T Medina, G M Luke, J Munevar, S Cheung, T Goko, Y J Uemura, J E Greedan.   

Abstract

The B-site ordered double perovskite Ba2CaOsO6 was studied by dc magnetic susceptibility, powder neutron diffraction and muon spin relaxation methods. The lattice parameter is a = 8.3619(6) Å at 280 K and cubic symmetry [Formula: see text] is retained to 3.5 K with a = 8.3462(7) Å. Curie-Weiss susceptibility behaviour is observed for T > 100 K and the derived constants are C = 0.3361(3) emu K mol(-1) and ΘCW = -156.2(3) K, in excellent agreement with literature values. This Curie constant is much smaller than the spin-only value of 1.00 emu K mol(-1) for a 5d(2) Os(6+) configuration, indicating a major influence of spin-orbit coupling. Previous studies had detected both susceptibility and heat capacity anomalies near 50 K but no definitive conclusion was drawn concerning the nature of the ground state. While no ordered Os moment could be detected by powder neutron diffraction, muon spin relaxation (µSR) data show clear long-lived oscillations indicative of a continuous transition to long-range magnetic order below TC = 50 K. An estimate of the ordered moment on Os(6+) is ∼ 0.2 μB, based upon a comparison with µSR data for Ba2YRuO6 with a known ordered moment of 2.2 μB. These results are compared with those for isostructural Ba2YReO6 which contains Re(5+), also 5d(2), and has a nearly identical unit cell constant, a = 8.36278(2) Å-a structural doppelgänger. In contrast, Ba2YReO6 shows ΘCW = - 616 K, and a complex spin-disordered and, ultimately, spin-frozen ground state below 50 K, indicating a much higher level of geometric frustration than in Ba2CaOsO6. The results on these 5d(2) systems are compared to recent theory, which predicts a variety of ferromagnetic and antiferromagnetic ground states. In the case of Ba2CaOsO6, our data indicate that a complex four-sublattice magnetic structure is likely. This is in contrast to the spin-disordered ground state in Ba2YReO6, despite a lack of evidence for structural disorder, for which theory currently provides no clear explanation.

Entities:  

Year:  2014        PMID: 25001885     DOI: 10.1088/0953-8984/26/30/306003

Source DB:  PubMed          Journal:  J Phys Condens Matter        ISSN: 0953-8984            Impact factor:   2.333


  3 in total

1.  Doping Evolution of the Local Electronic and Structural Properties of the Double Perovskite Ba2Na1-x Ca x OsO6.

Authors:  Jagadesh Kopula Kesavan; Dario Fiore Mosca; Samuele Sanna; Francesco Borgatti; Götz Schuck; Phuong Minh Tran; Patrick M Woodward; Vesna F Mitrović; Cesare Franchini; Federico Boscherini
Journal:  J Phys Chem C Nanomater Interfaces       Date:  2020-07-08       Impact factor: 4.126

2.  Spin-orbit coupling control of anisotropy, ground state and frustration in 5d(2) Sr2MgOsO6.

Authors:  Ryan Morrow; Alice E Taylor; D J Singh; Jie Xiong; Steven Rodan; A U B Wolter; Sabine Wurmehl; Bernd Büchner; M B Stone; A I Kolesnikov; Adam A Aczel; A D Christianson; Patrick M Woodward
Journal:  Sci Rep       Date:  2016-08-30       Impact factor: 4.379

3.  Revisiting Goodenough-Kanamori rules in a new series of double perovskites LaSr1-xCaxNiReO6.

Authors:  Somnath Jana; Payel Aich; P Anil Kumar; O K Forslund; E Nocerino; V Pomjakushin; M Månsson; Y Sassa; Peter Svedlindh; Olof Karis; Vasudeva Siruguri; Sugata Ray
Journal:  Sci Rep       Date:  2019-12-04       Impact factor: 4.379

  3 in total

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