@Article{DhruvMPCJBPMRB:2020:InStMa,
author = "Dhruv, Preksha N. and Meena, Sher Singh and Pullar, Robert C. and
Carvalho, Francisco E. and Jotania, Rajshree B. and Bhatt, Pramod
and Prajapat, C. L. and Machado, Jo{\~a}o Paulo Barros and Rao,
T. V. Chandrasekhar and Basak, C. B.",
affiliation = "{Gujarat University} and {Bhabha Atomic Research Centre} and
{University of Aveiro} and {Instituto Tecnol{\'o}gico de
Aeron{\'a}utica (ITA)} and {Gujarat University} and {Bhabha
Atomic Research Centre} and {Bhabha Atomic Research Centre} and
{Instituto Nacional de Pesquisas Espaciais (INPE)} and {Bhabha
Atomic Research Centre} and {Homi Bhabha National Institute}",
title = "Investigation of structural, magnetic and dielectric properties of
gallium substituted Z-type Sr3Co2-xGaxFe24O41 hexaferrites for
microwave absorbers",
journal = "Journal of Alloys and Compounds",
year = "2020",
volume = "822",
pages = "e153470",
month = "may",
keywords = "Gallium substituted Z-type hexaferrites, Sol-gel auto-combustion,
Structural properties, Magnetic properties, Microwave absorption
performance.",
abstract = "Gallium substituted Z-type hexagonal ferrites with chemical
composition Sr3Co2-xGaxFe24O41 (x ¼ 0.0,0.4, 0.8, 1.2, 1.6, and
2.0) were successfully synthesised in air at 1200 C for 5 h using
the sol-gel autocombustion technique, in order to investigate the
effect of gallium substitution on structural, magnetic and
dielectric properties. X-ray Diffraction (XRD) analysis of all
samples reveals the formation of mixed hexaferrite phases, with Z
ferrite as the major phase (72e90%).The average crystallite size
of heated powders was found to be in the range of 21e40 nm. The
saturation magnetisation decreases after gallium substitution,
with the lowest values of 64 Am2 kg1 for composition x ¼ 1.6,
which also hasthe highest value of coercivity (28.3 kA m1 ).
Nevertheless, all were soft ferrites, with Hc between 3.4 and 28.3
kA m1 .The Mr/MS ratio of all samples was found to be less than
0.5, suggesting that all the compositions possess multi-domain
microstructures. Mossbauer spectroscopic analysis con firmed that
the Fe ions were found in the 3 þ high spin state for compositions
below x 0.4, whereas ~1.5% of the Fe ions were converted into Fe2þ
high spin state beyond x 0.8 compositions, as Ga3þ began to
substitute for Fe3þ, forming Fe2þ in the cobalt positions. The
average hyperfine magnetic field (<Hhf>) was found to be decreased
with Ga-substitution. Dielectric parameters such as dielectric
constant and loss factor were studied as a function of frequency,
and their results show normal behaviour for ferrimagnetic
materials. In complex measurements at microwave frequencies (8
GHze12.5 GHz, the X-band), all samples had a real permittivity of
around 8e14. For sample x ¼ 2.0, a dielectric resonance peak was
observed around 12.15 GHz. All showed a real permeability of
around 1.0e1.4 over the frequency of 8 GHze12.5 GHz range, and
ferromagnetic resonance (FMR) was observed in x ¼ 0.0 and 2.0
samples, at around 11 and 12 GHz, respectively. This suggests that
the prepared samples can be used as microwave absorbers/EMI
shielding at specific microwave frequencies. The co-existence of
FMR and dielectric resonance at the same frequency of 12.15 GHz
for x ¼ 2.0 could lead to the coupling of these resonances and the
development of potential metamaterials.",
doi = "10.1016/j.jallcom.2019.153470",
url = "http://dx.doi.org/10.1016/j.jallcom.2019.153470",
issn = "0925-8388",
language = "en",
targetfile = "dhruv_investigation.pdf",
urlaccessdate = "27 abr. 2024"
}