2010
DOI: 10.1016/j.jmmm.2010.05.062
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Determination of intrinsic FMR line broadening in ferromagnetic (Fe44Co56)77Hf12N11 nanocomposite films

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Cited by 16 publications
(3 citation statements)
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“…FMR is also an informative technique to investigate the internal spin dynamics responsible for the relaxation processes in ferromagnetic nanoparticle systems. [8][9][10][11][12][13][14][15] Here, we describe the FMR studies of MgO:Ni to gain a physical insight into magnetic interactions and local anisotropy field phenomena.…”
Section: Introductionmentioning
confidence: 99%
“…FMR is also an informative technique to investigate the internal spin dynamics responsible for the relaxation processes in ferromagnetic nanoparticle systems. [8][9][10][11][12][13][14][15] Here, we describe the FMR studies of MgO:Ni to gain a physical insight into magnetic interactions and local anisotropy field phenomena.…”
Section: Introductionmentioning
confidence: 99%
“…Magneto-optic (Paz, 2012), dipolar energy contributions (Bose, 2012), nanocrystalline (Maklakov, 2012;Raita, 2012), La0.7Sr0.3MnO3 films (Golosovsky, 2012), La0.67Ba0.33Mn1-yA y O3, A -Fe, Cr , voltage-controlled magnetic anisotropy (VCMA) and spin transfer torque (Zhu, 2012) and the typical properties of the inertial resonance are investigated (Olive, 2012). The exchange bias (Backes, 2012), Q cavities for magnetic material (Beguhn, 2012), MgO/CoFeB/Ta structure , the interfacial origin of the giant magnetoresistive effect (GMR) phenomenon (Prieto, 2012), selfdemagnetization field (Hinata, 2012), Fe3O4/InAs(100) hybrid spintronic structures (Huang, 2012), granular films (Kakazei, 1999(Kakazei, , 2001Sarmiento, 2007;Krone, 2011;Kobayashi, 2012), nano-sized powdered barium (BaFe12O19) and strontium (Sr Fe12O19) hexaferrites (Korolev, 2012), Ni0.7Mn0.3-x CoxFe2O4 ferrites (NiMnCo: x = 0.00, 0.04, 0.06, and 0.10) (Lee, 2012), thin films (Demokritov, 1996(Demokritov, ,1997Nakai, 2002;Lindner, 2004;Aswal, 2005;Jalali-Roudsar, 2005;Cochran, 2006;Mizukami, 2007;Seemann, 2010), Ni2MnGa films (Huang, 2004), magnetic/electronic order of films (Shames, 2012), Fe1-xGd(Tb)x films , in ε-Al0.06Fe1.94O3 (Yoshikiyo, 2012). 10 nm thick Fe/GaAs(110) film (Römer, 2012), triangular shaped permalloy rings (Ding, 2012) and Co2-Y hexagonal ferrite single rod (Bai, 2012) structures and properties have been studied by FMR tecniques (Spaldin, 2010).…”
Section: Introductionmentioning
confidence: 99%
“…9(c) shows the FMR linewidth (Δ H ) as a function of applied operating frequency ( f ) for all the magnetic oxide samples. The observed data were fitted to a line by considering the Landau–Lifshitz–Gilbert (LLG) model represented by eqn (6) ; 101,102 where α is the Gilbert damping constant known as the intrinsic damping parameter. Δ H 0 is the frequency independent ( f = 0) contribution to Δ H produced by inhomogeneous broadening also called as extrinsic contribution to linewidth.…”
Section: Resultsmentioning
confidence: 99%