Issue 14, 2023

Microwave absorption property of GO–Fe/FeO–NiO HNFs: GO decorated Fe/FeO–NiO hexagonal flakes with a 2D/0D/2D structure

Abstract

In this study, Fe/FeO–NiO HNFs in which 2D NiO hexagonal nanoflakes (NiO HNFs) were decorated by 0D Fe/FeO NPs were prepared by a facile hydrothermal method. Then, 0D/2D Fe/FeO–NiO HNFs were loaded on 2D GO sheets in three different weight ratios of GO (1 : 3), (1 : 4), and (1 : 5) to Fe/FeO–NiO HNFs and a novel GO–Fe/FeO–NiO HNF composite with a 2D/0D/2D structure was successfully produced. TEM images revealed the interesting morphology of the GO–Fe/FeO–NiO HNF composite in which individual FeO NPs with a narrow size distribution (∼15 nm) were arranged in hexagonal NiO nanoflakes, decorated on the GO substrate. Since the morphology of nanomaterials has an important effect on their microwave absorption properties, designing a composite with an asymmetric morphology, which is the combination of zero, one, and two-dimensional nanostructures can be very efficient for adjusting the microwave absorption property. The microwave absorption ability of GO–Fe/FeO–NiO HNF composites was surveyed. All samples of Fe/FeO–NiO HNF composites exhibited superior microwave attenuation performance in terms of reflection loss with a suitable bandwidth. The minimum reflection losses for GO–Fe/FeO–NiO HNFs (1 : 3), (1 : 4), and (1 : 5) reached −75.22, −53, and −18 dB, respectively, and the effective absorption bandwidths (RL ≤ −10 dB) for GO–Fe/FeO–NiO HNFs (1 : 3), (1 : 4), and (1 : 5) were 2, 3 and 3.2 GHz, respectively.

Graphical abstract: Microwave absorption property of GO–Fe/FeO–NiO HNFs: GO decorated Fe/FeO–NiO hexagonal flakes with a 2D/0D/2D structure

Article information

Article type
Paper
Submitted
02 Mar 2023
Accepted
06 Mar 2023
First published
07 Mar 2023

Phys. Chem. Chem. Phys., 2023,25, 9925-9934

Microwave absorption property of GO–Fe/FeO–NiO HNFs: GO decorated Fe/FeO–NiO hexagonal flakes with a 2D/0D/2D structure

M. Arabi, S. M. Baizaee and H. Hekmatara, Phys. Chem. Chem. Phys., 2023, 25, 9925 DOI: 10.1039/D3CP00977G

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