A single phase polycrystalline La0.5Ba0.5CoO3-d sample possessing cubic structure (space group Pm3m) was synthesized by microwave irradiation within 20 minutes of processing time and its structural, magnetic, electrical, and magnetostrictive properties were investigated. While the temperature dependence of field-cooled magnetization (M) in a field of H = 0.5 kOe indicates the onset of ferromagnetic transition at T-C = 177 K, irreversibility between the zero field-cooled and field cooled M(T) persists even at H = 3 kOe. M(H) at 10 K does not saturate at the maximum available field and has a much smaller value (0.83 mu(B)/Co in a field of 50 kOe) than 1.9 mu(B)/Co expected for spin only contribution from intermediate Co3+ and Co4+ spins. Resistivity shows insulating behavior down to 10 K and only a small magnetoresistance (similar to; -2% for H = 70 kOe) occurs around T-C. All these results suggest a magnetically heterogeneous ground state with weakly interacting ferromagnetic clusters coexisting with a non-ferromagnetic phase. The length of the sample expands in the direction of the applied magnetic field (positive magnetostriction) and does not show saturation even at 50 kOe. The magnetostriction has a maximum value (lambda(par) = 265 x 10(-6)) at 10 K and it decreases with increasing temperature. The smaller value of lambda(par) compared to the available data on La0.5Sr0.5CoO3 (lambda(par) = 900 x 10(-6)) suggests that the non-ferromagnetic matrix is most likely antiferromagnetic and it restrains the field-induced expansion of ferromagnetic clusters in the microwave synthesized La0.5Ba0.5CoO3-d sample.& nbsp;(C) 2022 Author(s).All article content, except where otherwise noted, is licensed under a Creative Commons Attribution (CC BY)license (http://creativecommons.org/licenses/by/4.0/).
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Chinese Acad Sci, High Field Magnet Lab, Hefei 230031, Peoples R ChinaChinese Acad Sci, High Field Magnet Lab, Hefei 230031, Peoples R China
Zhang, Shile
Pi, Li
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Chinese Acad Sci, High Field Magnet Lab, Hefei 230031, Peoples R China
Univ Sci & Technol China, Hefei Natl Lab Phys Sci Microscale, Hefei 230026, Peoples R ChinaChinese Acad Sci, High Field Magnet Lab, Hefei 230031, Peoples R China
Pi, Li
Tong, Wei
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Chinese Acad Sci, High Field Magnet Lab, Hefei 230031, Peoples R ChinaChinese Acad Sci, High Field Magnet Lab, Hefei 230031, Peoples R China
Tong, Wei
Tan, Shun
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Univ Sci & Technol China, Hefei Natl Lab Phys Sci Microscale, Hefei 230026, Peoples R ChinaChinese Acad Sci, High Field Magnet Lab, Hefei 230031, Peoples R China
Tan, Shun
Zhang, Changjin
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Chinese Acad Sci, High Field Magnet Lab, Hefei 230031, Peoples R ChinaChinese Acad Sci, High Field Magnet Lab, Hefei 230031, Peoples R China
Zhang, Changjin
Zhang, Yuheng
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Chinese Acad Sci, High Field Magnet Lab, Hefei 230031, Peoples R China
Univ Sci & Technol China, Hefei Natl Lab Phys Sci Microscale, Hefei 230026, Peoples R ChinaChinese Acad Sci, High Field Magnet Lab, Hefei 230031, Peoples R China