Wetting and spreading of Ca‐Y‐Ba‐Cu‐O solution on Y2O3 and CaSZ crucible in growing Y1‐xCaxBa2Cu3O7‐δ single crystal

Sizable and uniform Y1‐xCaxBa2Cu3O7‐δ single crystals are of significant importance to study high‐temperature superconductivity. However, the severe liquid loss resulting from intrinsic wetting property during top‐seeded solution‐growth (TSSG), makes it difficult to obtain such crystals. Here the re...

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Veröffentlicht in:Journal of the American Ceramic Society 2020-09, Vol.103 (9), p.4859-4866
Hauptverfasser: Huang, Simin, Zhu, Yanhan, Qian, Jun, Wan, Yan, Yin, Yiqian, Zhou, Ligang, Diko, Pavel, Kucharova, Veronika, Zmorayova, Katarina, Kim, Young‐June, Yao, Xin
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container_end_page 4866
container_issue 9
container_start_page 4859
container_title Journal of the American Ceramic Society
container_volume 103
creator Huang, Simin
Zhu, Yanhan
Qian, Jun
Wan, Yan
Yin, Yiqian
Zhou, Ligang
Diko, Pavel
Kucharova, Veronika
Zmorayova, Katarina
Kim, Young‐June
Yao, Xin
description Sizable and uniform Y1‐xCaxBa2Cu3O7‐δ single crystals are of significant importance to study high‐temperature superconductivity. However, the severe liquid loss resulting from intrinsic wetting property during top‐seeded solution‐growth (TSSG), makes it difficult to obtain such crystals. Here the reactive wetting performance of the Ca‐Y‐Ba‐Cu‐O solution on two types of crucibles was studied. It was identified that the spreading process on the Y2O3 crucible is characterized by forming double‐layer of Y2BaCuO5 and YBa2Cu3O7‐δ, while that on the CaSZ crucible (Ca‐stabilized ZrO2) produces the BaZrO3 layer with CuO phase. In the former case, the liquid has a low energy interface with the top layer of YBa2Cu3O7‐δ, leading to strong spreading and creeping behaviors. Conversely, due to a high interfacial energy between solution and BaZrO3, the CaSZ crucible has a low wettability, particularly beneficial to solve the liquid loss problem. Consequently, with negligible liquid creeping out of CaSZ crucibles, we succeeded in growing a series of homogeneous Y1‐xCaxBa2Cu3O7‐δ single crystals with an acceptable size up to a × b × c = 11.2 × 11 × 4.8 mm3. Moreover the wetting modes of solution on various kinds of crucibles for TSSG in growing doped YBa2Cu3O7‐δ single crystals were also elucidated. Most importantly, the understanding gained from this work is broadly applicable for producing other desirable doped‐crystals. The reactive wetting and spreading performance of the Ca‐Y‐Ba‐Cu‐O solution on Y2O3 and Ca stabilized ZrO2 crucibles.
doi_str_mv 10.1111/jace.17212
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However, the severe liquid loss resulting from intrinsic wetting property during top‐seeded solution‐growth (TSSG), makes it difficult to obtain such crystals. Here the reactive wetting performance of the Ca‐Y‐Ba‐Cu‐O solution on two types of crucibles was studied. It was identified that the spreading process on the Y2O3 crucible is characterized by forming double‐layer of Y2BaCuO5 and YBa2Cu3O7‐δ, while that on the CaSZ crucible (Ca‐stabilized ZrO2) produces the BaZrO3 layer with CuO phase. In the former case, the liquid has a low energy interface with the top layer of YBa2Cu3O7‐δ, leading to strong spreading and creeping behaviors. Conversely, due to a high interfacial energy between solution and BaZrO3, the CaSZ crucible has a low wettability, particularly beneficial to solve the liquid loss problem. Consequently, with negligible liquid creeping out of CaSZ crucibles, we succeeded in growing a series of homogeneous Y1‐xCaxBa2Cu3O7‐δ single crystals with an acceptable size up to a × b × c = 11.2 × 11 × 4.8 mm3. Moreover the wetting modes of solution on various kinds of crucibles for TSSG in growing doped YBa2Cu3O7‐δ single crystals were also elucidated. Most importantly, the understanding gained from this work is broadly applicable for producing other desirable doped‐crystals. 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However, the severe liquid loss resulting from intrinsic wetting property during top‐seeded solution‐growth (TSSG), makes it difficult to obtain such crystals. Here the reactive wetting performance of the Ca‐Y‐Ba‐Cu‐O solution on two types of crucibles was studied. It was identified that the spreading process on the Y2O3 crucible is characterized by forming double‐layer of Y2BaCuO5 and YBa2Cu3O7‐δ, while that on the CaSZ crucible (Ca‐stabilized ZrO2) produces the BaZrO3 layer with CuO phase. In the former case, the liquid has a low energy interface with the top layer of YBa2Cu3O7‐δ, leading to strong spreading and creeping behaviors. Conversely, due to a high interfacial energy between solution and BaZrO3, the CaSZ crucible has a low wettability, particularly beneficial to solve the liquid loss problem. Consequently, with negligible liquid creeping out of CaSZ crucibles, we succeeded in growing a series of homogeneous Y1‐xCaxBa2Cu3O7‐δ single crystals with an acceptable size up to a × b × c = 11.2 × 11 × 4.8 mm3. Moreover the wetting modes of solution on various kinds of crucibles for TSSG in growing doped YBa2Cu3O7‐δ single crystals were also elucidated. Most importantly, the understanding gained from this work is broadly applicable for producing other desirable doped‐crystals. 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source Wiley Online Library Journals Frontfile Complete
subjects Barium zirconates
Crucibles
crystal growth
interface
Interfacial energy
Single crystals
Superconductivity
superconductors
Wettability
Wetting
YBCO superconductors
Yttrium oxide
Zirconium dioxide
title Wetting and spreading of Ca‐Y‐Ba‐Cu‐O solution on Y2O3 and CaSZ crucible in growing Y1‐xCaxBa2Cu3O7‐δ single crystal
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