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Mitglied der Helmholtz-Gemeinschaft Study of hexaferrite Ba0.6Sr1.4Zn2Fe12O22 by EPR technique Giorgi Khazaradze Tbilisi, July10, 2014 What is Multiferroics? Ferroelectric and Ferromagnetic orderings Schematic picture of Multiferroic Read with GMR MF-RAM Cycloidal spin ordering Mitglied der Helmholtz-Gemeinschaft Multiferroic Magnetoelectric effect P=α H M=α E D. Khomshii, Physics 2, 20 (2009) Write with a voltage Pij=eij x (si x sj) Dzyaloshinskii-Morya interaction [M. Bibes and A. Barthélémy, Nat. Mater. 7, 425 (2008)] 2 Mitglied der Helmholtz-Gemeinschaft Type of hexaferrites Schematic crystal structures of hexaferrites. The (110) cross section views of an M-type (Ba,Sr)Fe12O19, W-type (Ba,Sr)Me2 Fe16O27, X-type (Ba,Sr)2 Me2Fe28 O46 , Y-type (Ba,Sr)2Me2 Fe12O22, Z-type (Ba,Sr)3Me2 Fe24 O41 , and U-type (Ba,Sr)4Me2Fe36O60 with the c axis vertical. The (Fe,Me)-O-(Fe,Me) bond angles surrounded by dashed blue ellipsoids are strongly affected by the ratio of Sr to Ba. Kimura et al., Annu. Rev. Condens.Matter Phys. 2012. 3:93–110] 3 Mitglied der Helmholtz-Gemeinschaft a b c d a) cristal sructure, b-d magnetic structure of Y-type hehaferrite. b) The proper-screw, c) the transverse-conical, d) the conical 4 Kimura et al., Annu. Rev. Condens.Matter Phys. 2012. 3:93–110] Mitglied der Helmholtz-Gemeinschaft Magnetic field dependence of electric polarization at different Temperatures and magnetic phase diagram of High-T MF hexaferrite Ba0.5Sr1.5Zn2Fe12O22 with magnetic field perpendicular to 5 the c axis T. Kimura et al. Phys Rev. Lett. 94,137201 (2005) Short description of EPR • • • Zeeman splitting by magnetic field. 9.6 GHz electromagnetic wave is absorbed. Linewidth of EPR is caused by the interaction between the ions. Ez=h𝝂=gµβH Mitglied der Helmholtz-Gemeinschaft Ez −Zeeman energy 𝝂 − 𝑡ℎ𝑒 𝑓𝑟𝑒𝑞𝑢𝑒𝑛𝑦 𝑜𝑓 the microwave field Idea: apply electric field modulation and try to detect magnetic resonance in ME materials H=H‘+HmSin(2π𝝂mt) H‘−𝑺𝒕𝒂𝒕𝒊𝒄 𝒂𝒑𝒑𝒍𝒊𝒆𝒅 𝒎𝒂𝒈𝒏𝒆𝒕𝒊𝒄 field Hm−Modulation amplitude 𝝂m−Modulation frequency 𝝂m−100KHz P(t)=PmSin(2π𝝂mt) Mitglied der Helmholtz-Gemeinschaft P(t) –Detected absorbed power Schematic picture of the experiment and the Magnetic/Electric field directions A. Maisuradze Aet al., Phys. Rev. Lett., 108, 247211 (2012). Mitglied der Helmholtz-Gemeinschaft Electric-field modulated FMR is selectively sensitive to Magnetoelectric coupling in Cu2OSeO3 Temperature dependence of FMR signals of single-crystal Cu2OSeO3 detected using the MFM technique and the EFM technique A. Maisuradze et al., Phys. Rev. Lett., 108, 247211 (2012). Ferromagnetic resonance in Y-type hexaferrite Ba0.6Sr1.4Zn2Fe12O22 0.3 FMR Signal, a.u. Ba0.6Sr1.4Zn2Fe12O22 0.1 T=293K 0.0 -0.1 -0.2 -0.3 0 2000 4000 6000 Magnetic Field, G Mitglied der Helmholtz-Gemeinschaft H C axis 8000 Resonance field, G 7500 0.2 B C 6000 Ba0.6Sr1.4Zn2Fe12O22 T=293K 4500 3000 1500 0 15 30 45 60 75 Angle , Degree Angular dependence of the resonance field θ 9 Ferromagnetic resonance in Y-type hexaferrite Ba0.6Sr1.4Zn2Fe12O22 with Electric field modulation 0.25 Amplitude of firs FMR Line Amplitude of firs FMR Line 100 T=293K 0 -100 -200 Ba0.6Sr1.4Zn2Fe12O22 T=273K 0.15 0.10 0.05 -300 2000 4000 6000 8000 Magnetic Field, G Mitglied der Helmholtz-Gemeinschaft 0.20 Ba0.6Sr1.4Zn2Fe12O22 Amplitude, a.u FMR Signal, a.u. 200 FMR signal at Electric field 500 1000 1500 2000 2500 Electric field, V The amplitude of FMR signal as function Electric field 10 Magnetic and Electric Field Modulated FMR (EFMR) in Ba0.6Sr1.4Zn2Fe12O22 0.6 Magnetic Electric 0.2 FMR Signal, a.u. FMR Signal, a.u. 0.4 Ba0.6Sr1.4Zn2Fe12O22 0.0 0 =60 T=293K -0.2 Ba0.6Sr1.4Zn2Fe12O22 0.4 0 =90 T=293K 0.2 0.0 -0.2 -0.4 -0.4 0 2000 4000 6000 0 8000 Magnitoelectric coupling, Mitglied der Helmholtz-Gemeinschaft Magnetic Field, G 2000 4000 6000 Magnetic Field, G 8000 Coupling at second FMR line Coupling at first FMR line 1E-6 Ba0.6Sr1.4Zn2Fe12O22 T=293K T=293K 1E-7 1E-8 30 45 60 75 90 Angle , Degree 105 Angular dependence of the Magnetoelectric (ME) coupling 11 Summary and Conclusions • Ferromagnetic resonance (FMR) in Y-type hexaferrite single crystal Ba0.6Sr1.4Zn2Fe12O22 was observed. • Using electric field modulation FMR (EFMR) technique magnetoelectric coupling was observed in this compound. • Magnetoelectric coupling was estimated, however it is week at room temperature. • Magnetoelectric coupling was determined quantitatively as a function of temperature and magnetic field orientation. Mitglied der Helmholtz-Gemeinschaft Outlook • The next step would be to study this compound at lower temperatures and appropriate magnetic field range where electric polarization was observed by using Soft X-ray Scattering method. 12 Mitglied der Helmholtz-Gemeinschaft Thanks for your Attention! 13