首页> 外文期刊>Applied Superconductivity, IEEE Transactions on >High $J_{rm c}$ ${hbox {GdBa}}_{2}{hbox {Cu}}_{3}{hbox {O}}_{7-delta}$ Coated Conductors on ${hbox {CeO}}_{2}$-Buffered IBAD MgO Template Fabricated by Pulsed Laser Deposition
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High $J_{rm c}$ ${hbox {GdBa}}_{2}{hbox {Cu}}_{3}{hbox {O}}_{7-delta}$ Coated Conductors on ${hbox {CeO}}_{2}$-Buffered IBAD MgO Template Fabricated by Pulsed Laser Deposition

机译:高$ J_ {rm c} $ $ {hbox {GdBa}} _ {2} {hbox {Cu}} _ {3} {hbox {O}} _ {7-delta} $ $ {hbox {CeO }} _ {2}通过脉冲激光沉积制备的$缓冲IBAD MgO模板

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High quality ${hbox {GdBa}}_{2}{hbox {Cu}}_{3}{hbox {O}}_{7-delta}$ (GdBCO) coated conductors (CCs) were successfully fabricated on ${hbox {CeO}}_{2}$-buffered IBAD MgO template by pulsed laser deposition (PLD). With the same energy density of 2 J/cm$^{2}$, laser frequency of 8 Hz, and oxygen pressure of 300 mTorr, both target-to-substrate distance $(D_{rm ts})$ and substrate temperature $(T_{rm s})$ were systematically varied from 5.5 to 4.0 cm at $T_{rm s}$ of 780 $^{circ}{hbox {C}}$ and from 760 to 820 $^{circ}{hbox {C}}$ at $D_{rm ts}$ of 4.5 cm, respectively, to investigate their effects on the grain alignment, microstructure, and superconducting properties of GdBCO films. Biaxially aligned GdBCO films without $a$-axis oriented GdBCO grains could be deposited at $T_{rm s}$ higher than 780 $^{circ}{hbox {C}}$ and $D_{rm ts}$ shorter than 5.0 cm. At $T_{rm s}$ of 760 $^{circ}{hbox {C}}$, a small amount of $a$-axis oriented and 45$^{circ}$ misaligned GdBCO grains was formed. The in-plane textures of GdBCO films were gradually improved when $D_{rm ts}$ decreased, while those were first improved with increasing $T_{rm s}$ up to 800 $^{circ}{hbox {C}}$ and then degraded at 820 $^{circ}{hbox {C}}$. The highest critical current density $(J_{rm c})$ of 3.9 ${rm MA/cm}^{2}$ and critical current $(I_{rm c})$ of 195 A/cm-width (77 K, self-field) were achieved from the 500 nm GdBCO film deposited at 800$^{circ}{hbox {C}}$ with $D_{rm ts}$ of 4.5 cm . The $J_{rm c}$ values of GdBCO films were found to be sensitive to the in-plane texture and also to the presence of $a$ -axis oriented grains and 45$^{circ}$ misaligned grains.
机译:高质量$ {hbox {GdBa}} _ {2} {hbox {Cu}} _ {3} {hbox {O}} _ {7-delta} $(GdBCO)涂层导体(CC)成功地在$ { hbox {CeO}} _ {2} $通过脉冲激光沉积(PLD)缓冲的IBAD MgO模板。在2 J / cm $ ^ {2} $的相同能量密度,8 Hz的激光频率和300 mTorr的氧气压力下,目标到基板的距离$(D_ {rm ts})$和基板温度$ (T_ {rm s})$在780 $ ^ {circ} {hbox {C}} $的$ T_ {rm s} $和760至820 $ ^ {circ} {hbox {C}} $在$ D_ {rm ts} $分别为4.5厘米处,以研究它们对GdBCO薄膜的晶粒取向,微结构和超导性能的影响。没有$ a $轴取向的GdBCO晶粒的双轴取向GdBCO膜可以以高于780 $ ^ {circ} {hbox {C}} $和$ D_ {rm ts} $小于5.0的$ T_ {rm s} $沉积。厘米。在760个$ ^ {circ} {hbox {C}} $的$ T_ {rm s} $处,形成少量的$ a $轴取向和45 $ ^ {circ} $错位的GdBCO晶粒。当降低$ D_ {rm ts} $时,GdBCO膜的面内纹理逐渐改善,而随着提高$ T_ {rm s} $至800 $ ^ {circ} {hbox {C}} $然后降级为820 $ ^ {circ} {hbox {C}} $。最高临界电流密度$(J_ {rm c})$ 3.9 $ {rm MA / cm} ^ {2} $和临界电流$(I_ {rm c})$$ 195 A / cm宽度(77 K ,自场)是通过以800 ^ {circ} {hbox {C}} $和4.5 cm的D_ {rm ts} $沉积的500 nm GdBCO薄膜获得的。发现GdBCO膜的$ _ {rm c} $值对平面纹理以及轴取向的晶粒和45°未对准的晶粒的存在敏感。

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