Observation of exsolution textures within Ba–Cu–O-rich solidified melts of Y–Ba–Cu–O materials and their relationship to Y123 nucleation and texturing

Layers (about 60–100 μm thick) of almost pure BaCuO 2 (BC1), as determined using X-ray diffractometry (XRD) and scanning electron microscopy (SEM), coat the surfaces of YBa 2Cu 3O 7− x (Y123) samples partial melt processed using a single-zone vertical furnace. The actual Cu/Ba ratio of the BC1 phase...

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Bibliographic Details
Published inPhysica. C, Superconductivity Vol. 331; no. 3; pp. 201 - 215
Main Authors Alarco, J.A, Riches, J.D, Barry, J.C
Format Journal Article
LanguageEnglish
Published Elsevier B.V 01.05.2000
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Summary:Layers (about 60–100 μm thick) of almost pure BaCuO 2 (BC1), as determined using X-ray diffractometry (XRD) and scanning electron microscopy (SEM), coat the surfaces of YBa 2Cu 3O 7− x (Y123) samples partial melt processed using a single-zone vertical furnace. The actual Cu/Ba ratio of the BC1 phase is 1.2–1.3 as determined using energy dispersive X-ray spectrometry (EDS). The nominally BC1 phase displays an exsolution of BC1.5 or BC2 in the form of thin plates (about 50–100 nm thick) along {100}-type cleavage planes or facets. The exsolved phase also fills cracks within the BC1 layer that require it to be in a molten state at some stage of processing. The samples were influenced by Pt contamination from the supporting wire, which may have stabilised the BC1.5 phase. Many of the Y123 grains have the same morphology as the exsolution domains, and run nearly parallel to the thin plates of the exsolved phases, strongly indicating that Y123 nucleation took place at the interface between the BC1 and the BC1.5 or BC2 exsolved phases. The network of nearly parallel exsolved “channels” provides a matrix and a mechanism through which a high degree of local texture can be initiated in the material.
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ISSN:0921-4534
1873-2143
DOI:10.1016/S0921-4534(00)00023-X