2015
DOI: 10.1109/tasc.2014.2365407
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Growth Condition Dependence of Microcracks in YBCO Thin Films Pulsed Laser Deposited on <inline-formula> <tex-math notation="TeX">$\hbox{NdGaO}_{3}$</tex-math></inline-formula> (001) Substrates

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Cited by 3 publications
(3 citation statements)
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“…The introduction of nanocrystals in YBCO results in an increase in Ɛ00ℓ when they are homogeneously distributed throughout the layer (Table 1), and this in turn can be related to the enhanced pinning properties and Jc isotropy as previously reported by other groups. 12,15,17,[41][42][43][68][69] The increase of Ɛ00ℓ in the BZO, SZO and BHO nanocomposites results in a nearly linear increase of H * (Figure 7A) and a polynomial decrease of α (Figure 7B) at 77 K. Conversely, the BTO-added film has Ɛ00ℓ similar to the pristine film due to the agglomeration of BTO nanocrystals and therefore shows no improvement of pinning properties. Figure 7C shows a linear correlation between Ɛ00ℓ and the normalized Jc at 77K and 1 T as a consequence of the enhanced pinning properties.…”
Section: Relation Between Microstrain and Pinning Propertiesmentioning
confidence: 99%
“…The introduction of nanocrystals in YBCO results in an increase in Ɛ00ℓ when they are homogeneously distributed throughout the layer (Table 1), and this in turn can be related to the enhanced pinning properties and Jc isotropy as previously reported by other groups. 12,15,17,[41][42][43][68][69] The increase of Ɛ00ℓ in the BZO, SZO and BHO nanocomposites results in a nearly linear increase of H * (Figure 7A) and a polynomial decrease of α (Figure 7B) at 77 K. Conversely, the BTO-added film has Ɛ00ℓ similar to the pristine film due to the agglomeration of BTO nanocrystals and therefore shows no improvement of pinning properties. Figure 7C shows a linear correlation between Ɛ00ℓ and the normalized Jc at 77K and 1 T as a consequence of the enhanced pinning properties.…”
Section: Relation Between Microstrain and Pinning Propertiesmentioning
confidence: 99%
“…Superconductivity has found to be thickness dependent; therefore, precise control of thin films is crucial. Here, PLD provides an advantage of controlled growth of thin films through variation in experimental parameters [69,70], which can improve the quality of thin films in individual applications. There are many recent studies found in literature that demonstrate the exploration of experimental parameters of PLD for diverse types of highquality superconducting thin films.…”
Section: Pulsed Laser Depositionmentioning
confidence: 99%
“…Superconducting transition was observed around 12 K at a film thickness of 9 nm. One of the benefits of PLD method is that quality and thickness of thin films can be controlled by varying deposition time, growth rate (determined by pulse repetition rate) and substrate temperature during the film growth [69,70].…”
Section: Pulsed Laser Depositionmentioning
confidence: 99%