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Download Material for Temporary Copying Purposes Only, Provided These Uses Are for Noncommercial Personal Purposes Durham Research Online Deposited in DRO: 06 May 2015 Version of attached le: Other Peer-review status of attached le: Peer-reviewed Citation for published item: McCabe, E. E. and Wills, A. S. and Chapon, L. and Manuel, P. and Evans, J. S. O. (2014) 'Structural and magnetic characterization of iron oxyselenides Ce2O2Fe2OSe2 and Nd2O2Fe2OSe2.', Physical review B., 90 (16). p. 165111. Further information on publisher's website: http://dx.doi.org/10.1103/PhysRevB.90.165111 Publisher's copyright statement: Reprinted with permission from the American Physical Society: Physical Review B 90, 165111 c 2014 by the American Physical Society. Readers may view, browse, and/or download material for temporary copying purposes only, provided these uses are for noncommercial personal purposes. 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Durham University Library, Stockton Road, Durham DH1 3LY, United Kingdom Tel : +44 (0)191 334 3042 | Fax : +44 (0)191 334 2971 https://dro.dur.ac.uk Structural and magnetic characterisation of iron oxyselenides Ce2O2Fe2OSe2 and Nd2O2Fe2OSe2 E. E. McCabe,1, 2 A. S. Wills,3 L. Chapon,4, 5 P. Manuel,5 and J. S. O. Evans2 1School of Physical Sciences, University of Kent, Canterbury, CT2 7NH, UK 2Department of Chemistry, Durham University, Durham DH1 3LE, UK 3Department of Chemistry, University College London, 20 Gordon Street, London, WC1H 0AJ, UK 4Diffraction Group, Institute Laue Langevin, 71 avenue des Martyrs, 38000 Grenoble, France 5ISIS Facility, Rutherford Appleton Labs, Chilton Didcot, OX11 0QX, UK (Dated: October 21, 2014) We present here an investigation of the magnetic ordering in the Mott insulating oxyselenide materials Ln2O2Fe2OSe2 (Ln = Ce, Nd). Neutron powder diffraction data are consistent with a non-collinear multi-k ordering on the iron sublattice structure and analysis indicates a reduced 2+ 3+ magnetic correlation length perpendicular to the [Fe2O] layers. The magnetic role of the Ln cations is investigated and Ce3+ moments are found to order for T ≤ 16 K. ◦ 1. INTRODUCTION J20 180 Fe { O { Fe interactions) are fully satisfied. In- terestingly, a similar 2-k model, composed of perpendicu- lar AFM chains, has been predicted for the FeAs sheets in The discovery of iron-based superconductivity [1] in iron arsenides and oxyarsenides [27, 28]. The recent stud- several mixed anion systems has driven research to un- ies on La O Fe OSe indicated the presence of antiphase derstand the magnetism of these materials which is 2 2 2 2 boundaries or stacking faults perpendicular to the stack- related to their superconducting behaviour [2]. The ing direction and gave evidence for 2D-Ising-like mag- 1111 family of iron-based superconductors derive from netism within these sheets [25]. In the light of this work, LnFeAsO (Ln = trivalent lanthanide) and adopt the it is timely to report a similar analysis on Ln O Fe OSe ZrCuSiAs-structure [3], composed of alternating layers 2 2 2 2 (Ln = Ce, Nd) analogues to test the robustness of the of anti-fluorite-like edge-linked FeAs tetrahedra alter- 4 2-k model to changes in Fe { O bond lengths and to a nating with fluorite-like edge-linked OLn tetrahedra. 4 magnetic moment on the Ln site. We show that neutron Although the superconductivity arises in the iron ar- powder diffraction (NPD) data are consistent with the senide layers, the Ln3+ cation has a significant role in proposed 2-k magnetic structure and that much larger both tuning the superconducting T in the doped mate- c magnetic stacking domains are formed with these smaller rials [1, 4] and in defining the magnetism of the par- magnetic lanthanides. In contrast with previous work ent non-superconducting materials (such as the spin- [10], we show that Ce moments order at low tempera- reorientations in NdFeAsO [5] and PrFeAsO [6]). This tures and that unlike many related oxyarsenide systems, has led to much research into the interplay between tran- this Ce moment ordering does not cause a reorientation sition metal and lanthanide magnetic sublattices in these of the Fe2+ moments. and related mixed-anion systems [7{19]. La2O2Fe2OSe2 was the first reported member of the \M2O" (M = transition metal) family of oxyselenide 2. EXPERIMENTAL DETAILS materials and adopts a layered structure with fluorite- 2+ like [La2O2] slabs (analogous to those in 1111 iron 5 g each of Ce2O2Fe2OSe2 and Nd2O2Fe2OSe2 were 2− 2+ oxyarsenides) separated by Se anions from [Fe2O] prepared by solid state reaction of CeO2 (Alfa-Aesar, 2+ sheets (Figure 1) [20]. The Fe cations are coordi- 99.8%) or Nd2O3 (Electronic Materials, 99%), Fe nated by two O(2) ions within these anti-CuO2 sheets, (Aldrich, 99.9%) and Se (Alfa Aesar, 99.999%) pow- 2− and by four Se ions above and below the sheets, form- ders. For Nd2O2Fe2OSe2, stoichiometric quantities of arXiv:1410.4990v1 [cond-mat.str-el] 18 Oct 2014 ing a network of face-shared FeO2Se4 trans octahedra. these reagents were intimately ground by hand using Much research has been carried out to understand the an agate pestle and mortar. The resulting grey pow- exchange interactions and magnetic ordering present in der was pressed to form several pellets of 5 mm di- 2+ these [Fe2O] sheets [21]. La2O2Fe2OSe2 orders antifer- ameter. These were placed inside a quartz tube which romagnetically (AFM) below ∼ 90 K [22] and two mag- was evacuated and sealed. This was then heated slowly netic structures have been discussed: a 2-k model first to 1000◦C, held at this temperature for 12 hours and proposed for Nd2O2Fe2OSe2 [23] and a collinear model then cooled in the furnace. For Ce2O2Fe2OSe2, a sto- [10, 22]. Recent work suggests that the 2-k model is the ichiometric mixture of reagents were ground together more likely [24{26]. In this magnetic structure (Figure and pressed into pellets which were placed in a quartz 1), both next-nearest-neighbour (nnn) interactions (fer- tube with an oxygen-getter (Al powder in 10% excess ◦ romagnetic J2 ∼ 95 Fe { Se { Fe interactions, and AFM which was physically isolated from the reagents). This 2 1a) 1b) 1e) J O Se a 2’ Fe J La 2 O(1) Se J1 Fe O(2) b 1c) 4.10 La 4.08 Ce 4.06 / Å / Pr a 4.04 Nd 4.02 4.00 1.10 1.12 1.14 1.16 Ln3+ cation radius 1d) 18.60 Series1 EEM249e_1La EEM249e_2 Cava 18.50 Ce / Å / Pr c Nd 18.40 18.30 1.10 1.12 1.14 1.16 Ln3+ cation radius 2− 2− 2+ 3+ FIG. 1. [color online] a) nuclear cell of Ln2O2Fe2OSeSeries12 with O , Se EEM249e_1, Fe and Ln ions in red, yellow, blue and green, 2+ respectively, showing [Ln2O2] fluorite-like layers built from edge-shared OLn4 tetrahedra in red; b) shows the in-plane arrangement of magnetic moments for the 2-k model, with O2− (red) Se2− (yellow) and Fe2+ (blue) ions shown, and Fe2+ moments shown by blue arrows; the three intraplanar exchange interactions J1, J2 and J20 are also shown; c) and d) show plots of unit cell parameters a and c for Ln2O2Fe2OSe2 determined from Rietveld analysis using room temperature XRPD data (data in blue are described in this work including quench-cooled Ce2O2Fe2OSe2); data in red are determined for the main ( ) and secondary (×) phases in two phase samples of \Ce2O2Fe2OSe2"; green points are those reported for Ce2O2Fe2OSe2 by Ni et al [10]); e) illustrates the magnetic ordering of Ce (green) and Fe (blue) moments (O(1) sites are omitted for clarity). tube was evacuated, sealed, slowly heated to 1000◦C followed by a further five on warming to 300 K. Rietveld and held at this temperature for 12 hours. The reac- refinements [29] were performed using Topas Academic tion tube was then quenched into a bucket of iced water. software [30, 31]. Sequential refinements were controlled ◦ Both Ce2O2Fe2OSe2 and Nd2O2Fe2OSe2 were formed as using local subroutines. The high d-spacing 59 bank of black, polycrystalline powders. Preliminary structural data (10.5 { 85.0 ms, 1 { 8 A)˚ was used to study the mag- characterisation was carried out using a Bruker D8 Ad- netic behaviour of the two materials. The nuclear and vance diffractometer fitted with a LynxEye silicon strip magnetic refinements were carried out with separate nu- detector (step size 0.021◦) operating in reflection mode clear and magnetic phases (lattices parameters and scale with Cu Kα radiation. NPD data were collected on the factor of the magnetic phase were constrained to be mul- time of flight (TOF) diffractometer WISH on target sta- tiples of the nuclear phase). Magnetic susceptibility was tion 2 at the ISIS spallation neutron source. The powders measured using a Magnetic Properties Measurement Sys- were placed in cylindrical 6 mm diameter vanadium cans tem (Quantum Design, MPMS). Field-cooled and zero- (to heights of ∼6 cm). For Ce2O2Fe2OSe2, 16 minute field-cooled data were collected on warming from 2 K (10 µA h) scans were collected every 4 K on cooling from to 292 K at 5 K intervals in an applied magnetic field 120 K to 8 K and a final 25 minute (15 µA h) scan was of 1000 Oe.
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