TY - JOUR
T1 - Effect of nio nanoparticle addition on the structural, microstructural, magnetic, electrical, and magneto-transport properties of la0.67 ca0.33 mno3 nanocomposites
AU - Lau, Lik Nguong
AU - Lim, Kean Pah
AU - Chok, See Yee
AU - Ishak, Amirah Natasha
AU - Hon, Xiao Tong
AU - Wong, Yan Jing
AU - Awang Kechik, Mohd Mustafa
AU - Chen, Soo Kien
AU - Ibrahim, Noor Baa’Yah
AU - Miryala, Muralidhar
AU - Murakami, Masato
AU - Shaari, Abdul Halim
N1 - Funding Information:
This research was fully funded and supported by the Ministry of Higher Education, Malaysia (MOHE), through the Fundamental Research Grant Scheme (FRGS/1/2019/STG07/UPM/ 02/4) and a Universiti Putra Malaysia (UPM) research grant (GP-IPS/2018/9663900). The authors are grateful to the support staff who assisted in the characterisation measurements and for the facilities provided by UPM. L.N. is thankful to the Shibaura Institute of Technology, SIT as the host of aPBL under the Sakura Science Plan and facilitated some of the sample characterisation in this work.
Funding Information:
Funding: This research was fully funded and supported by the Ministry of Higher Education, Malaysia (MOHE), through the Fundamental Research Grant Scheme (FRGS/1/2019/STG07/UPM/ 02/4) and a Universiti Putra Malaysia (UPM) research grant (GP-IPS/2018/9663900).
Publisher Copyright:
© 2021 by the authors. Licensee MDPI, Basel, Switzerland.
PY - 2021/7
Y1 - 2021/7
N2 - Incorporation of the secondary oxide phase into the manganite composite capable of enhancing low-field magnetoresistance (LFMR) for viability in high-performance spintronic applica-tions. Polycrystalline La0.67 Ca0.33 MnO3 (LCMO) was prepared via the sol–gel route in this study. The structural, microstructural, magnetic, electrical, and magneto-transport properties of (1−x) LCMO: x NiO, x = 0.00, 0.05, 0.10, 0.15 and 0.20 were investigated in detail. The X-ray diffraction (XRD) patterns showed the coexistence of LCMO and NiO in the composites. The microstructural analysis indicated the amount of NiO nanoparticles segregated at the grain boundaries or on the surface of LCMO grains increased with the increasing secondary phase content. LCMO and NiO still retained their individual magnetic phase as observed from AC susceptibility (ACS) measurement. This further confirmed that there is no interfacial diffusion reaction between these two compounds. The NiO nanoparticle acted as a barrier to charge transport and caused an increase in resistivity for composite samples. The residual resistivity due to the grain/domain boundary is responsible for the scattering mechanism in the metallic region as suggested by the theoretical model fitting, ρ(T) = ρ0 + ρ2 T2 + ρ4.5 T4.5 . The magnetoresistance values of LCMO and its composites were found to increase monotonically with the decrease in temperature. Hence, the LFMR was observed. Nonetheless, the slight reduction of LFMR in composites was attributed to the thick boundary layer created by NiO and impaired the spin polarised tunnelling process.
AB - Incorporation of the secondary oxide phase into the manganite composite capable of enhancing low-field magnetoresistance (LFMR) for viability in high-performance spintronic applica-tions. Polycrystalline La0.67 Ca0.33 MnO3 (LCMO) was prepared via the sol–gel route in this study. The structural, microstructural, magnetic, electrical, and magneto-transport properties of (1−x) LCMO: x NiO, x = 0.00, 0.05, 0.10, 0.15 and 0.20 were investigated in detail. The X-ray diffraction (XRD) patterns showed the coexistence of LCMO and NiO in the composites. The microstructural analysis indicated the amount of NiO nanoparticles segregated at the grain boundaries or on the surface of LCMO grains increased with the increasing secondary phase content. LCMO and NiO still retained their individual magnetic phase as observed from AC susceptibility (ACS) measurement. This further confirmed that there is no interfacial diffusion reaction between these two compounds. The NiO nanoparticle acted as a barrier to charge transport and caused an increase in resistivity for composite samples. The residual resistivity due to the grain/domain boundary is responsible for the scattering mechanism in the metallic region as suggested by the theoretical model fitting, ρ(T) = ρ0 + ρ2 T2 + ρ4.5 T4.5 . The magnetoresistance values of LCMO and its composites were found to increase monotonically with the decrease in temperature. Hence, the LFMR was observed. Nonetheless, the slight reduction of LFMR in composites was attributed to the thick boundary layer created by NiO and impaired the spin polarised tunnelling process.
KW - Fitting
KW - Grain boundary
KW - LFMR
KW - Sol–gel
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U2 - 10.3390/coatings11070835
DO - 10.3390/coatings11070835
M3 - Article
AN - SCOPUS:85110919393
SN - 2079-6412
VL - 11
JO - Coatings
JF - Coatings
IS - 7
M1 - 835
ER -