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2016
DOI: 10.1016/j.nme.2016.03.004
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Irradiation performance of rare earth and nanoparticle enhanced high temperature superconducting films based on YBCO

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Cited by 11 publications
(6 citation statements)
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“…Except in very low magnetic fields, an initial increase in J c at low dose is followed by rapid decrease after a critical dose which depends on the type of conductor, measurement temperature and type of projectile. The initial improvement in J c has been associated with the introduction of additional non‐superconducting flux pinning centres, 12,13 and the subsequent rapid degradation due to both the increased rate of flux creep rate (caused by the reduced separation of flux pinning centres decreasing the activation barrier) 14 and the eventual loss of superconducting cross‐sectional area, 15 although no reliable method has been suggested to demonstrate or quantify this second effect. The effect of neutron irradiation on superconducting critical temperature ( T c ) has also been studied and showed a linear reduction in T c with a slope of approximately 3% per 1 × 10 22 n/m 2 fluence is reported, 16,17 but the width of the superconductor/normal transition temperature is unchanged 18 .…”
Section: Introductionmentioning
confidence: 99%
“…Except in very low magnetic fields, an initial increase in J c at low dose is followed by rapid decrease after a critical dose which depends on the type of conductor, measurement temperature and type of projectile. The initial improvement in J c has been associated with the introduction of additional non‐superconducting flux pinning centres, 12,13 and the subsequent rapid degradation due to both the increased rate of flux creep rate (caused by the reduced separation of flux pinning centres decreasing the activation barrier) 14 and the eventual loss of superconducting cross‐sectional area, 15 although no reliable method has been suggested to demonstrate or quantify this second effect. The effect of neutron irradiation on superconducting critical temperature ( T c ) has also been studied and showed a linear reduction in T c with a slope of approximately 3% per 1 × 10 22 n/m 2 fluence is reported, 16,17 but the width of the superconductor/normal transition temperature is unchanged 18 .…”
Section: Introductionmentioning
confidence: 99%
“…Great efforts have been made to introduce artificial defects as pinning centers into RE123 thin films to improve the I c of RE123 CCs. [3][4][5][6] Among these defects, Y124-type SFs are frequently observed, due to additional randomly distributed Cu-O stacking faults inserted into the Y123 matrix to form a Y124-type structure. It is believed that the evolution of Y124-type SFs can be attributed to an inadequate reaction or insufficient ion diffusion during the growth of RE123 films, especially when the ex situ metal-organic deposition (MOD) method is used.…”
mentioning
confidence: 99%
“…Альтернативным методом создания искусственных центров пиннинга являются радиационные воздействия. На практике используется облучение нейтронами [31][32][33][34][35][36][37][38], протонами [39], электронами [40], γ-квантами [41] и тяжелыми ионами [42]. Помимо возможности создания дополнительных центров пиннинга при малых концентрациях дефектов, радиационное воздействие привлекательно тем, что, используя ионное облучение с энергиями порядка 1−10 МeV, можно создать концентрации дефектов, существенно изменяющие критический ток и критическую температуру вплоть до полной потери сверхпроводимости.…”
Section: Introductionunclassified