Effect of Co <sup>2+</sup> substitution on the structural, terahertz and magnetic characterization of NiZn ferrites
Meenakshi Arya, Mayuri Gandhi, S. S. Prabhu, Venu Gopal Achanta, Siddhartha P. Duttagupta
Abstract
Abstract We present detailed studies on spinel structured Ni 0.5 Co x Zn 0.5− x Fe 2 O 4 ( x = 0.1, 0.2 and 0.3), synthesized by sol–gel combustion method. In addition to the structural properties, we present optical dielectric and magnetic response of this system as a function of x . From x-ray diffraction analysis, a single-phase formation in cubic spinel structure was confirmed with an average crystallite size ( D avg ) variation of 46–61 nm. X-ray diffractograms were analyzed to evaluate the lattice constant ( a ), x-ray density ( ρ x ) and porosity ( P ) in percentage. Energy dispersive x-ray spectroscopy was used to delimit the compositional mass ratios. Terahertz (THz) time-domain spectroscopy measurements were performed to investigate the refractive index ( <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:msub> <mml:mover> <mml:mi>n</mml:mi> <mml:mo stretchy="false">ˆ</mml:mo> </mml:mover> <mml:mrow> <mml:mtext>s</mml:mtext> </mml:mrow> </mml:msub> </mml:math> ) of the samples at room temperature in a frequency range from 0.2 to 2.5 THz. Real and imaginary components of complex optical dielectric constant ( <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:msub> <mml:mrow> <mml:mover> <mml:mi>ε</mml:mi> <mml:mo stretchy="false">ˆ</mml:mo> </mml:mover> </mml:mrow> <mml:mrow> <mml:mtext>s</mml:mtext> </mml:mrow> </mml:msub> </mml:math> ) with the increase of Co 2+ content were deduced using THz spectroscopy data. The complex optical dielectric constant for the substitution of Co 2+ content at x = 0.1, 0.2 and 0.3, was determined within 5% error ∼9.6 + i0.07, ∼10.9 + i0.2 and ∼11.7 + i0.5, respectively. The magnetic measurements were performed at a temperature range of 300–50 K using a superconducting quantum interference device vibrating sample magnetometer under an applied magnetic field of ±5 tesla. We found the highest saturation magnetization ( M s ) of about 86.7 emu g −1 , 83.5 emu g −1 and 80.4 emu g −1 for the substitution of Co 2+ content at x = 0.1, 0.2 and 0.3, respectively at room temperature.