Ferromagnetic resonance of facing-target sputtered epitaxial γ′-Fe4N films: the influence of thickness and substrates

The microstructure and high frequency properties of facing-target sputtered epitaxial γ′-Fe4N films were investigated in detail. It was found that the eddy current in ultrathin γ′-Fe4N films is too small to influence the ferromagnetic resonance (FMR) linewidth, where the linewidth is mostly determined by intrinsic damping and the two-magnon scattering (TMS) process. In relatively thick films, the TMS process can significantly affect the linewidth due to the roughness on the sample surface. However, the TMS process in a thin film is quite weak because of its smooth surface. The Gilbert damping constant of about 0.0135 in our γ′-Fe4N films is smaller than the experimental value in the previous work. Moreover, substrates can also influence the FMR linewidth of the γ′-Fe4N films by the TMS process. Besides, the resonance field of polycrystalline γ′-Fe4N film is larger than the epitaxial ones because of the lack of a magnetic anisotropic field, but the linewidth of the polycrystalline γ′-Fe4N film is smaller.

[1]  Ankit Kumar,et al.  Temperature-dependent Gilbert damping of Co2FeAl thin films with different degree of atomic order , 2017, 1706.04670.

[2]  Supriyo Bandyopadhyay,et al.  Static and Dynamic Magnetic Properties of Sputtered Fe–Ga Thin Films , 2017, IEEE Transactions on Magnetics.

[3]  Ming Liu,et al.  Spin-orbital coupling induced four-fold anisotropy distribution during spin reorientation in ultrathin Co/Pt multilayers , 2017 .

[4]  T. Suemasu,et al.  Growth and magnetic properties of epitaxial Fe4N films on insulators possessing lattice spacing close to Si(001) plane , 2016 .

[5]  Shishen Yan,et al.  Broad-Band FMR Linewidth of Co 2 MnSi Thin Films with Low Damping Factor: The Role of Two-Magnon Scattering , 2016 .

[6]  T. Silva,et al.  Radiative damping in waveguide-based ferromagnetic resonance measured via analysis of perpendicular standing spin waves in sputtered permalloy films , 2015, 1508.05265.

[7]  Weisheng Zhao,et al.  Tunnel Junction with Perpendicular Magnetic Anisotropy: Status and Challenges , 2015, Micromachines.

[8]  W. Mi,et al.  Anisotropic magnetoresistance in facing-target reactively sputtered epitaxial γ′-Fe4N films , 2015 .

[9]  J. Zhu,et al.  Medium Optimization for Lowering Head Field and Heating Requirements in Heat-Assisted Magnetic Recording , 2015, IEEE Magnetics Letters.

[10]  Ming Liu,et al.  Voltage Tuning of Ferromagnetic Resonance and Linewidth in Spinel Ferrite/Ferroelectric Multiferroic Heterostructures , 2015, IEEE Magnetics Letters.

[11]  H. Bai,et al.  Inversion of exchange bias and complex magnetization reversal in full-nitride epitaxial γ′-Fe4N/CoN bilayers , 2015 .

[12]  L. Alff,et al.  Growth, structure, and magnetic properties of γ′-Fe4Nγ′-Fe4N thin films , 2015 .

[13]  M. Oogane,et al.  Dependence of Magnetic Damping on Temperature and Crystal Orientation in Epitaxial Fe4N Thin Films , 2014 .

[14]  Tao Liu,et al.  Ferromagnetic resonance of sputtered yttrium iron garnet nanometer films , 2014 .

[15]  H. Bai,et al.  Reactively sputtered epitaxial γ′-Fe4N films: Surface morphology, microstructure, magnetic and electrical transport properties , 2013 .

[16]  T. Suemasu,et al.  Negative spin polarization at the Fermi level in Fe4N epitaxial films by spin-resolved photoelectron spectroscopy , 2012 .

[17]  Sung-chul Shin,et al.  Enhanced magnetic moment of epitaxial γ′-Fe4N films at low temperature , 2012 .

[18]  H. Akinaga,et al.  Spin and orbital magnetic moments of molecular beam epitaxy γ′-Fe4N films on LaAlO3(001) and MgO(001) substrates by x-ray magnetic circular dichroism , 2011 .

[19]  A. Sakuma,et al.  Inverse Current-Induced Magnetization Switching in Magnetic Tunnel Junctions with Fe4N Free Layer , 2010 .

[20]  J. Park,et al.  Analysis of oxidation behavior of the β-Nb phase formed in Zr–1.5Nb alloy by using the HVEM , 2009 .

[21]  T. Suemasu,et al.  Spin polarization of Fe4N thin films determined by point-contact Andreev reflection , 2009 .

[22]  M. Takahashi,et al.  75% inverse magnetoresistance at room temperature in Fe4N/MgO/CoFeB magnetic tunnel junctions fabricated on Cu underlayer , 2009 .

[23]  C. Patton,et al.  Microwave damping in polycrystalline Fe-Ti-N films: Physical mechanisms and correlations with composition and structure , 2008 .

[24]  T. Suemasu,et al.  Growth of Nitride-Based Fe3N/AlN/Fe4N Magnetic Tunnel Junction Structures on Si(111) Substrates , 2007 .

[25]  M. Takahashi,et al.  Inverse tunnel magnetoresistance in magnetic tunnel junctions with an Fe4N electrode , 2007 .

[26]  Michael L. Schneider,et al.  Ferromagnetic resonance linewidth in metallic thin films: Comparison of measurement methods , 2006 .

[27]  Heiko Wende,et al.  Two-magnon scattering and viscous Gilbert damping in ultrathin ferromagnets , 2006 .

[28]  R. McMichael,et al.  Classical model of extrinsic ferromagnetic resonance linewidth in ultrathin films , 2004, IEEE Transactions on Magnetics.

[29]  C. Patton,et al.  Optimized pulsed laser deposited barium ferrite thin films with narrow ferromagnetic resonance linewidths , 2003 .

[30]  H. Bai,et al.  Structure and magnetic properties of facing-target sputtered Co-C granular films , 2003 .

[31]  U. Ebels,et al.  Ferromagnetic resonance studies of Ni nanowire arrays , 2001 .

[32]  K. Niihara,et al.  Formation and photoluminescence of Ge and Si nanoparticles encapsulated in oxide layers , 2000 .

[33]  R. Arias,et al.  Extrinsic contributions to the ferromagnetic resonance response of ultrathin films , 1999 .

[34]  M. Farle Ferromagnetic resonance of ultrathin metallic layers , 1998 .

[35]  Zbigniew Celinski,et al.  Ferromagnetic resonance linewidth of Fe ultrathin films grown on a bcc Cu substrate , 1991 .

[36]  A. Stoneham Linewidths with gaussian and lorentzian broadening , 1972 .

[37]  E. Schlömann Inhomogeneous Broadening of Ferromagnetic Resonance Lines , 1969 .

[38]  J. Lock Eddy current damping in thin metallic ferromagnetic films , 1966 .