2021
DOI: 10.1016/j.matpr.2020.12.650
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Effect of Gd3+ substitution on the structural and magnetic properties of barium hexaferrite nanomaterials

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Cited by 15 publications
(2 citation statements)
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“…Sharma et al analyzed the effect of Gd 3+ doping in M-type barium hexaferrites. This article describes the effect of induced lattice strain due to Gd 3+ substitution presenting another way to control magnetic properties [21]. Multi substitution in barium hexaferrites has also been utilized extensively to achieve desired magnetic properties e.g.…”
Section: Introductionmentioning
confidence: 99%
“…Sharma et al analyzed the effect of Gd 3+ doping in M-type barium hexaferrites. This article describes the effect of induced lattice strain due to Gd 3+ substitution presenting another way to control magnetic properties [21]. Multi substitution in barium hexaferrites has also been utilized extensively to achieve desired magnetic properties e.g.…”
Section: Introductionmentioning
confidence: 99%
“…Phase composition was analyzed by X‐ray diffraction (XRD, D/max 2200 PC, Rigaku, Tokyo, Japan) using Cu Ka radiation at the diffraction angles 2θ ranging from 10° to 90° with a scan speed of 4°/min. Some specimens and Si powders used as external standard were analyzed by XRD with a slow scan speed of 1°/min and a scan step of 0.02°, in order to perform Rietveld refinement by FullProf software and calculate the lattice strain by MDI Jade software (Version 6.5, Materials Data, Inc., USA) based on the Williamson–Hall (W‐H) equation: 44,45 βhklcosθbadbreak=kλ/Dgoodbreak+4sinθ\begin{equation}{\beta }_{hkl}\cos \theta = k\lambda /D + 4\sin \theta \end{equation}where β hkl is the peak full width at half maximum intensity (FWHM) excluding the instrumental FWHM, D , k , λ , and ε are crystallite size, shape factor, the wavelength of CuK α1 radiation, and lattice strain, respectively. The phases were further identified by Raman spectroscopy (Renishaw‐InVia, Renishaw, UK) with the 532 nm argon laser.…”
Section: Methodsmentioning
confidence: 99%