Synthesis and Characterization of SmBa2Cu3Oy Powder Prepared by Solid-State Reaction

2020 ◽  
Vol 12 (2) ◽  
pp. 180-185
Author(s):  
Paitoon Boonsong ◽  
Pimpilai Wannasut ◽  
Chakrit Sriprachuabwong ◽  
Adisorn Tuantranont ◽  
Anucha Watcharapasorn

In this work, the SmBa2Cu3Oy (Sm-123) powder was successfully prepared by solid-state reaction method under a normal air atmosphere using a stoichiometric ratio (i.e., Sm:Ba:Cu = 1:2:3) of high-purity Sm2O3, BaCO3 and CuO starting powders. Thermal properties of the as-calcined powder were studied by DSC/TGA technique and the results showed a formation of Sm-123 phase at 900 °C. The as-calcined powder was prepared by heating the starting precursors at 900 °C for 6–30 h. Phase identification was determined using an X-ray diffractometer (XRD). The quantitative phase analysis was analyzed by fitting the XRD pattern using the GSAS-II program. The result of XRD showed that the SmBa2 Cu3Oy (Sm-123) was identified as the main crystalline phase. The morphology was observed by scanning electron microscopy (SEM) with chemical composition identification from EDS mode. The surface of Sm-123 powder exhibited large agglomerates with a size range of ∼4.44–6.75 m. The Raman spectra showed a vibrational Raman-active phonon mode lying at around ∼502–508 cm–1. The peaks originated from the apical oxygen O(4) (i.e., O(4)-Ag mode) along the c-axis could be correlated with the oxygen deficiency in the CuO2 planes of orthorhombic SmBa2Cu3Oy. The calculated oxygen content from these peaks tended to decrease with increasing calcination time. All of these frequencies confirmed the presence of phonon and bonding typical for the 123-type structure.

2019 ◽  
Vol 891 ◽  
pp. 224-229
Author(s):  
Naphat Albutt ◽  
Vanussanun Aitviriyaphan ◽  
Thanapong Sareein ◽  
Sudarath Suntaropas ◽  
Panakamon Thonglor ◽  
...  

The magnetic properties of Ba2FeMoO6 (BFMO) double perovskite are investigated. BFMO samples were prepared by solid state reaction method through compression. Magnetic properties are influenced by electron environments of the Fe3+ and Mo5+ ions within the perovskite structure. BFMO sintered at 800 oC exhibited the largest hysteresis loop at 50 K. In addition, the values of Ms and Mr indicate ferromagnetic behaviour in BFMO ceramics sintered at 800 oC for different times up to 10 hours. Using the Curie-Weiss law fitting to investigate μeff~30μB high spin of Fe and Mo, and negative θ present the antiferromagnetic characteristics of the BFMO sample.


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