Abstract:Using a novel melt-spinning technique, we have produced both amorphous and nanocrystalline NdBa~Cu307-~ and GdBa2C~307-~ materials. Samples melt-spun in 0 2 consist' of nanocrystals with the tetragonal 123 structure while those processed in N2 show an amorphous matrix with small amounts of crystalline BaCu202, as shown by XRD and TEM studies. The difference is due to the strong dependence of the phase relations on the 0 2 partial pressure. Superconductivity can be fully restored by heating above 1000°C followe… Show more
“…Moreover, the amorphouslike phase was more reactive to the atmospheric gasses than the Nd123 phase, which is subject to decomposition. [9][10][11] As discussed in Sec. This is also associated with the fact that XRD results at room temperature did not indicate any distinct features of the amorphous phase.…”
Section: Discussionmentioning
confidence: 99%
“…[9][10][11] It was suggested that the amorphous phase was obtained and the Nd123 phase crystallized from the amorphous phase around 630°C by high-temperature x-ray diffrac-tion (HTXRD) at heating condition of 6.5°C/min. [9][10][11] It was suggested that the amorphous phase was obtained and the Nd123 phase crystallized from the amorphous phase around 630°C by high-temperature x-ray diffrac-tion (HTXRD) at heating condition of 6.5°C/min.…”
Small spherical samples (diameter approximately 2 mm) of NdBa 2 Cu 3 O 7−␦ (Nd123) were fully melted in Ar gas flow in an aero-acoustic levitation device and subsequently rapidly cooled by splat quenching. For samples quenched above the liquidus, the microstructual and x-ray-diffraction (XRD) observations suggested the existence of the amorphous phase with small quantities of the BaCuO 2 and BaCu 2 O x . The high-temperature XRD results indicated that the decomposition of the amorphous phase, probably assisted by atmospheric CO 2 and H 2 O, led to formation of the BaCO 3 phase at 400°C and, subsequently, the Nd123 phase was formed by the solid diffusion above 800°C. Another set of Nd123 samples was fully melted in O 2 gas flow, undercooled while levitated, and then splat quenched at a temperature below the peritectic temperature (T P ). These samples possessed a microcrystalline microstructure of the Nd123 phase that was confirmed by XRD. This indicated that the Nd123 phase was solidified directly from the undercooled melt quenched below T P .
“…Moreover, the amorphouslike phase was more reactive to the atmospheric gasses than the Nd123 phase, which is subject to decomposition. [9][10][11] As discussed in Sec. This is also associated with the fact that XRD results at room temperature did not indicate any distinct features of the amorphous phase.…”
Section: Discussionmentioning
confidence: 99%
“…[9][10][11] It was suggested that the amorphous phase was obtained and the Nd123 phase crystallized from the amorphous phase around 630°C by high-temperature x-ray diffrac-tion (HTXRD) at heating condition of 6.5°C/min. [9][10][11] It was suggested that the amorphous phase was obtained and the Nd123 phase crystallized from the amorphous phase around 630°C by high-temperature x-ray diffrac-tion (HTXRD) at heating condition of 6.5°C/min.…”
Small spherical samples (diameter approximately 2 mm) of NdBa 2 Cu 3 O 7−␦ (Nd123) were fully melted in Ar gas flow in an aero-acoustic levitation device and subsequently rapidly cooled by splat quenching. For samples quenched above the liquidus, the microstructual and x-ray-diffraction (XRD) observations suggested the existence of the amorphous phase with small quantities of the BaCuO 2 and BaCu 2 O x . The high-temperature XRD results indicated that the decomposition of the amorphous phase, probably assisted by atmospheric CO 2 and H 2 O, led to formation of the BaCO 3 phase at 400°C and, subsequently, the Nd123 phase was formed by the solid diffusion above 800°C. Another set of Nd123 samples was fully melted in O 2 gas flow, undercooled while levitated, and then splat quenched at a temperature below the peritectic temperature (T P ). These samples possessed a microcrystalline microstructure of the Nd123 phase that was confirmed by XRD. This indicated that the Nd123 phase was solidified directly from the undercooled melt quenched below T P .
“…[3][4][5][6][7] One particularly interesting finding is that the substitution of Nd and other RE elements for yttrium, either full or partial, has been found to have little or no deleterious effect on the electronic properties of the material. A great deal of work has been put into fully characterizing REsubstituted 1:2:3 in terms of the crystal structure and the phase transformations that occur.…”
Drop-tube experiments have been performed on Y x Nd 1−x Ba 2 Cu 3 O y (0.7 ഛ x ഛ 1.0) to understand the effects of partial substitutions of Nd for Y on the phase relationships in these systems at elevated temperatures. Powders 50-100 m in diameter were processed in pure O 2 at furnace temperatures of 1575-1800°C, every 25°C. The resulting samples were examined microstructurally by scanning electron microscopy, energy dispersive spectroscopy, and optical microscopy. Powder x-ray diffraction was performed for phase identification. It was found that Nd substitution alters phase selection by introducing at least one new phase and allowing for solidification of the superconducting composition directly from the melt via undercooling to below the peritectic transformation temperature. A decreasing trend in the overall melting temperature with increasing Nd was also identified.
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