The Study of Temperature-Dependent Magnetic Properties Variation in CoCr2O4 Nanoparticles with (y = 0.8) and Without Coating Concentration of Non-Magnetic (SiO2)y

Author:

Mehboob Ghazanfar1ORCID,Nadeem Kashif2,Iqbal Amjad3ORCID,Mehboob Gohar4,Hussain Shahnawaz5,Ragab Mohamed6ORCID,Iqbal Mazhar7,Ajmal Sohaib8ORCID,El-Marghany Adel6ORCID

Affiliation:

1. 1 State Key Laboratory for Mechanical Behavior of Materials, School of Materials Science and Engineering , Xi’an Jiaotong University , Xi’an , , China

2. 2 Department of Physics , International Islamic University Islamabad , Pakistan

3. 3 Faculty of Materials Engineering , Sileisan University of Technology , Gliwice , Poland

4. 4 School of Materials Science and Engineering , South China University of Technology , Guangzhou , China

5. 5 Department of Mechanical Engineering (Production and Design), Shoubra Faculty of Engineering , Benha University , Benha , Egypt

6. 6 Department of Physics , University Azad Jammu and Kashmir , Muzaffarabad , Pakistan

7. 7 Institute for Advanced Ceramics, School of Materials Science and Engineering, Harbin Institute of Technology , Harbin , China

8. 8 Department of Chemistry , College of Science, King Saud University , P.O. Box 2455 , Riyadh , Saudi Arabia

Abstract

Abstract The present study investigates the temperature-dependent magnetic (MT) properties of CoCr2O4/(SiO2)y (y = 0 and 0.8) nanoparticles. Nanoparticles were synthesised by using the conventional sol–gel technique. The X-ray diffraction (XRD) method confirmed the normal spinel structure of CoCr2O4 nanoparticles. The main peak analysis of the XRD pattern using Debye–Scherrer’s formula probes the mean crystallite sizes for coated and uncoated nanoparticles, and the sizes based on which the probes have been carried out amount to 19 nm and 28 nm, respectively. The transmission electron microscopy (TEM) image showed the non-spherical shape of these nanoparticles. Field-cooled (FC) and zero field-cooled (ZFC) MT plots were taken by using a superconducting quantum interference device (SQUID) magnetometer. Pure CoCr2O4 nanoparticles showed the ferrimagnetic transition at Curie temperature (Tc = 99 K) on an applied field (H) of 50 Oe. Tc decreased up to 95 K with the increase in 80% SiO2 concentration in CoCr2O4 nanoparticles. For pure samples, conical spiral temperature (TS) and lock-in transition temperature (TL) remain unchanged with increasing magnetic field because of strong spin–lattice coupling. However, for 80% SiO2 impurity, the decrease in Tc was attributed to the reduction in surface disorder with a minor decline in TS and TL. The Ms declined with a decrease in temperature because of the existence of stiffed/strong conical spin-spiral and lock-in states in pure CoCr2O4 nanoparticles, while nanoparticles with 80% coating SiO2 concentration showed abnormal behavior. The coercivity increases with a decrease in temperature due to a decrease in thermal fluctuations at low temperatures for both samples. The fitting of coercivity (Hc) versus temperature plot by using Kneller’s law has given the values of coercivity constant (α) and coercivity at average blocking temperature (TB) for both samples, which are α = 0.54, TB = 75 K and α = 1.59, TB = 81 K, respectively. Hence, the increase in the concentration of SiO2 decreased nanoparticles size and surface disorder in CoCr2O4 nanoparticles while enhancing Ms below spin-spiral state ordering.

Publisher

Walter de Gruyter GmbH

Subject

Mechanical Engineering,Control and Systems Engineering

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