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21#
發(fā)表于 2025-3-25 05:56:08 | 只看該作者
22#
發(fā)表于 2025-3-25 09:47:29 | 只看該作者
https://doi.org/10.1007/978-3-658-08615-2s the most universal method and enables crystals to be prepared from compounds melting with decomposition, experiencing reconstructive phase transitions at extremely high temperatures, etc. Other methods of growing these crystals are not always feasible. Secondly, the flux method is most interesting
23#
發(fā)表于 2025-3-25 12:34:14 | 只看該作者
Charles F. Andrain,David E. Apterdies on the search for, synthesis of, and determination of the physical characteristics of an enormous number of various oxides mainly based on cuprates. The first result of this broad search was the observation of yttrium-alkaline-earth superconductors with higher transition temperatures into the s
24#
發(fā)表于 2025-3-25 15:50:02 | 只看該作者
25#
發(fā)表于 2025-3-25 21:43:47 | 只看該作者
https://doi.org/10.1057/9781137291622eir properties. An important part of this activity is the investigation of the growth mechanism of HTSC layers and the effect of the microstructure on their electro-physical properties. The perfection of the crystalline structure of the grains and the presence of intermediate phases seem to determin
26#
發(fā)表于 2025-3-26 02:35:37 | 只看該作者
27#
發(fā)表于 2025-3-26 05:41:46 | 只看該作者
https://doi.org/10.1007/978-3-658-43982-8per, including those grown with a large cross section. The wetting angle is maximal in the Stepanov method with a wetted shaper. In these variations, the meniscus remains low. For this reason, the growth process becomes more stable and the melt is fed well from the crucible through the shaper capillary.
28#
發(fā)表于 2025-3-26 10:54:40 | 只看該作者
29#
發(fā)表于 2025-3-26 15:34:05 | 只看該作者
30#
發(fā)表于 2025-3-26 20:41:19 | 只看該作者
Local Shaping and Growth from the Melt of Intricate Sapphire Articles on “Crystallization Center” Eqions of a millimeter, without detaching the meniscus from the shaper edge. If the meniscus detaches from the edge, the growth becomes unstable and a given crystal shape is in general not reproducible [2].
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