Location via proxy:   [ UP ]  
[Report a bug]   [Manage cookies]                
  • Editors' Suggestion

Intrinsic exchange bias in ZnxMn3xO4 (x1) solid solutions

Daniel P. Shoemaker, Efrain E. Rodriguez, Ram Seshadri, Ivana Sabaj Abumohor, and Thomas Proffen
Phys. Rev. B 80, 144422 – Published 26 October 2009

Abstract

Bulk specimens of the hetærolite solid solution ZnxMn3xO4 with x=0, 0.25, 0.5, 0.75, and 1 have been prepared as homogeneous, phase-pure polycrystalline samples as ascertained by neutron-diffraction measurements. Samples with x=0.25, 0.5, and 0.75 exhibit shifted magnetic hysteresis loops at low temperature, characteristic of exchange bias typically seen in magnetic composites. We propose that the unusual magnetic behavior arises as a result of a nanoscale mixture of ferrimagnetic and antiferromagnetic regions that are distinct but lack long-range order. While some glassy behavior is seen in ac magnetic measurements, its magnitude is not sufficient to account for the observed dramatic exchange bias. Furthermore, isothermal and thermoremanent magnetization measurements distinguish this material from a pure spin glass. The title system offers insights into the alloying of a ferrimagnet Mn3O4 with an antiferromagnet ZnMn2O4 wherein distinct magnetic clusters grow and percolate to produce a smooth transition between competing orders.

  • Figure
  • Figure
  • Figure
  • Figure
  • Figure
  • Figure
  • Figure
5 More
  • Received 22 June 2009

DOI:https://doi.org/10.1103/PhysRevB.80.144422

©2009 American Physical Society

Authors & Affiliations

Daniel P. Shoemaker*, Efrain E. Rodriguez, and Ram Seshadri

  • Materials Department and Materials Research Laboratory, University of California, Santa Barbara, California 93106, USA

Ivana Sabaj Abumohor

  • Centro para la Investigación Interdisciplinaria Avanzada en Ciencia de los Materiales, Departamento de Ingeniería Química y Biotecnología, Universidad de Chile, Casilla 2777, Santiago, Chile

Thomas Proffen

  • Los Alamos National Laboratory, Lujan Neutron Scattering Center, MS H805, Los Alamos, New Mexico 87545, USA

  • *dshoe@mrl.ucsb.edu

Article Text (Subscription Required)

Click to Expand

References (Subscription Required)

Click to Expand
Issue

Vol. 80, Iss. 14 — 1 October 2009

Reuse & Permissions
Access Options
Author publication services for translation and copyediting assistance advertisement

Authorization Required


×

Images

  • Figure 1
    Figure 1
    300 K neutron TOF diffraction Rietveld refinements in the I41/amd space group confirm the purity of all ZnxMn3xO4 phases at 300 K. Difference profiles are shown below each fit. Refinement results (including Rwp) are provided in Table .Reuse & Permissions
  • Figure 2
    Figure 2
    Structural parameters at 300 K from neutron TOF Rietveld refinements show decreasing (a) c/a ratios and (b) cell volume with Zn concentration (linear fits, dashed), due to its smaller radius. The oxygen z position in (c) decreases toward the undistorted value of 0.25. In (d), chemical disorder causes compounds with intermediate Zn/Mn mixing to have higher thermal parameters than the end members. Error bars are smaller than the symbols in all panels.Reuse & Permissions
  • Figure 3
    Figure 3
    (Color online) Neutron TOF powder diffraction patterns (log scale, offset for clarity) for the ZnxMn3xO4 solid solutions at 300, 50, and 20 K. The Rietveld fit to the 300 K (nonmagnetic) profile is shown for all samples. Note that only diffuse magnetic scattering is evident around d=5Å, for the sample with x=0.5. In Mn3O4, the baseline at 20 K drops due to transfer of diffuse magnetic scattering to Bragg peaks. Structural peaks in Mn3O4 are indexed using the standard I41/amd cell, while magnetic peaks () are indexed using the doubled magnetic cell (a, 2a, c) of Jensen and Nielsen.(Ref. 29).Reuse & Permissions
  • Figure 4
    Figure 4
    (Color online) The ZnMn2O4 hetærolite unit cell is shown in (a) with oxygen polyhedra drawn around Mn (red octahedra) and Zn (blue tetrahedra). In (b), the B-site linkages are shown. The BB direct exchange net consists of a stretched pyrochlore lattice (four interwoven kagomé nets) with BB links in a and b directions (dark) that are shorter than those with a c component (light). The diamond-type A lattice is shown in (c).Reuse & Permissions
  • Figure 5
    Figure 5
    FC and ZFC magnetization curves at H=1000Oe for the ZnxMn3xO4 solid solution show a gradual decrease in the magnetic ordering temperature, as well as the magnetization from x=0 to 1. The interactions in ZnMn2O4 are antiferromagnetic changes cannot be observed on this magnetization scale; these shown in greater detail in Fig. 6.Reuse & Permissions
  • Figure 6
    Figure 6
    Inverse susceptibility ZFC/FC data (a) for ZnMn2O4 shows Curie-Weiss behavior above room temperature with a very broad, gradual ordering of the spins that begins around 260 K. Small amounts of irreversibility are seen in (b), which indicates a magnetic transition at T=60K. In (c), the appearance of a magnetic Bragg peak in TOF neutron data between 100 and 50 K indicates the onset of long-range magnetic order coinciding with the peak in (b). The antiferromagnetic downturn in this sample only occurs at near 40 K. The Rietveld fit at 100 K is for structural peaks only.Reuse & Permissions
  • Figure 7
    Figure 7
    (Color online) Curie-Weiss normalization of the FC magnetization curves provides a view of the differing magnetic ordering schemes in the ZnxMn3xO4 solid solution. Deviation from purely paramagnetic behavior (dashed) is ferrimagnetic for samples with x<1, with TC decreasing with the number of A-site spins. Only ZnMn2O4 has antiferromagnetic ordering at low temperature.Reuse & Permissions
  • Figure 8
    Figure 8
    The Curie-Weiss temperature Θ versus composition (a) shows increasing dominance of short-range antiferromagnetic interactions as the solid solution progresses from Mn3O4 to ZnMn2O4. The dotted line is a guide to the eye. The paramagnetic μeff shown in (b) begins below the ideal L+S contribution (dashed line) for Mn3O4, but increases past the expected value for ZnMn2O4. This increase in effective moment with x is counterintuitive since Mn2+ spins are being removed, but could be attributed to Jahn-Teller orbital ordering contributions.Reuse & Permissions
  • Figure 9
    Figure 9
    Hysteresis loops (a–c) measured at 5 K after HFC=+50kOe field-cooling show dramatic exchange-biased loop shifts. The x=0.75 and 0.5 loops are pinned so that the coercive field HC in the +H direction is zero. This results in overlapping values of loop shift HE and half loop width HC versus temperature (d–f). Some shift is still evident in x=0.25 and disappears in Mn3O4.Reuse & Permissions
  • Figure 10
    Figure 10
    TRM and IRM versus applied field for a x=0.5 sample shows clear deviation up to H=50kOe. Lines are guides to the eye. For a typical spin glass, the two curves should join with increasing H as the field aligns the disordered moments to saturation. In an exchange-biased system, the curves remain separated as seen here.Reuse & Permissions
  • Figure 11
    Figure 11
    (Color online) Magnetic ac susceptibility for with mixed tetrahedral occupancy: (a) Zn0.25Mn2.75O4, (b) Zn0.5Mn2.5O4, and (c) Zn0.75Mn2.25O4. The ac field is 1 Oe with different dc fields shown. Local maxima in (a) and (b) are marked with symbols and replotted in (d) to show de Almeida-Thouless behavior. No such trend is present in (c), where maxima are present only at the ferrimagnetic TC around 18 K. Spin-glass freezing temperatures Tf and critical fields Hcr can be extracted for both curves in (d): for Zn0.25Mn2.75O4 Tf=36.9K and Hcr=5320Oe; for Zn0.5Mn2.5O4 Tf=20.6K and Hcr=2020Oe.Reuse & Permissions
  • Figure 12
    Figure 12
    (Color online) The ac magnetic susceptibility for Zn0.5Mn2.5O4 exhibits frequency dependence in the region associated with spin glass freezing. The T value of the maximum is plotted versus f in the inset. Error bars are smaller than the data points. The variation of Tf with f agrees with standard spin-glass behavior. The Tg extracted from this data differs from that in Fig. 11 due to the large nonglassy ferrimagnetic contribution.Reuse & Permissions
×

Sign up to receive regular email alerts from Physical Review B

Log In

Cancel
×

Search


Article Lookup

Paste a citation or DOI

Enter a citation
×