Abstract:
In the present study, M-Cr (M = Co, Ni, Cu, Zn and Mn) substituted magnesium
ferrite nanomaterials (Mg1-xMxCrxFe2-xO4 with x = 0.0-0.5) have been prepared by the
polyethylene glycol assisted micro-emulsion method. Thermal and XRD analyses
reveal that the complete spinel cubic phase formation occurred at 1123 K. The
average crystallite sizes in differently doped series are in the range of 15-62 nm. The
micrographs obtained from SEM analysis show that the synthesized materials are
agglomeration of the individual particles. The energy dispersive X-Ray fluorescence
(ED-XRF) spectrometric analysis reveals that the observed molar ratios of different
components of the samples are in close agreement with their nominal compositions.
Variation of Mössbauer parameters is explained on the basis of preferential site
occupancy of the substituted cations. The center shift (CS) value for A-site is smaller
than that of B-site due to difference in the Fe3+-O2- inter-nuclear separation, normally
larger for B-site as compared to that for A-site. The value of quadrupole splitting (QS)
is negligibly small which indicates that the overall symmetry of Fe3+ surroundings is
not disturbed with the substitution of the dopant ions into a magnesium ferrite matrix.
With the increase of dopant contents, the variations of hyperfine magnetic field (H)
and site population area (A) are akin to the compositional variation of saturation
magnetization, MS. Symmetric magnetic hysteresis loops are measured using a
superconducting quantum interference device (SQUID) magnetometer up to an
applied magnetic field of 50 kOe at 300, 200 and 100 K. SQUID analysis reveals
narrow hysteresis loops with a coercivity (HC) and saturation magnetization (MS)
varying for different compositions. The high field regimes of these loops are modeled
using the Law of Approach (LoA) to saturation to extract information regarding
magnetocrystalline anisotropy and saturation magnetization. In the present study, the
saturation magnetization of magnesium ferrite increases by doping with Co-Cr, Ni-Cr,
Zn-Cr and Mn-Cr, respectively, but decreases by doping with Cu-Cr contents. The
coercivity (HC) of all the series studied here decreases with an increase in the
substitution level. All the magnetic parameters i.e. MS, Mr, K1 and HC increase with
decrease in the temperature from 300 K to 100 K. To determine the Curie temperature
(TC), the temperature dependence of normalized moment is measured at an applied
field of 5 kOe within the temperature range of 350-973 K, using a vibrating-sample
magnetometer. The Curie temperature initially increases with Co-Cr and Mn-Cr
contents, but start to decrease for higher level of substitution. In case of Ni-Cr doped
series, TC value increases progressively with the increase in dopant contents, while it
continued to decrease with the substitution of Cu-Cr and Zn-Cr contents. Temperature
dependence of DC-electrical resistivity reflects the semi-conducting nature of the
doped Mg-ferrites. The room temperature resistivity (ρRT) and activation energy
increase up to a certain level of substitution with Ni-Cr, Zn-Cr and Mn-Cr contents
but increase continuously for Co-Cr and Cu-Cr substitution contents. The dielectric
constant (έ) and dielectric loss tangent (tan δ) decrease with increasing applied field
frequency. The variations in the magnitude of drift mobility, dielectric constant and
dielectric loss tangent are in close agreement with the trend of DC-electrical
resistivity by increasing the dopant contents. With improvement in properties, the
synthesized materials could be suitable for potential application in some magnetic and
microwave devices.