2019
DOI: 10.1088/1361-6668/ab5164
|View full text |Cite
|
Sign up to set email alerts
|

Competition between pinning produced by extrinsic random point disorder and superconducting thermal fluctuations in oxygen-deficient GdBa2Cu3O x coated conductors

Abstract: We report on the influence of random point defects introduced by 3 MeV proton irradiation on the vortex dynamics of 1.3 μm thick GdBa 2 Cu 3 O x coated conductors. Thin films with different oxygen stoichiometry (6.7<×<7) were irradiated with 3 MeV proton (p) using a fluence of 2×10 16 p cm −2 . We find a direct correlation between the changes in T c produced by oxygen content and damage by irradiation on the resulting vortex dynamics in the films. The analysis of the critical current densities J c at low… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1

Citation Types

0
1
0

Year Published

2021
2021
2023
2023

Publication Types

Select...
2

Relationship

0
2

Authors

Journals

citations
Cited by 2 publications
(1 citation statement)
references
References 36 publications
0
1
0
Order By: Relevance
“…phonons). However, for materials where the observed T c does not solely depend on the electron-phonon interaction (in particular, in cuprates [51,53,54], pnictides [75][76][77] and nickelates [78,79]), but instead on the thermodynamic fluctuations [58,[80][81][82][83], the presence of pseudogap [84,85], structural disorder [86][87][88][89], system dimensionality [90][91][92][93][94] or other mechanisms [95][96][97][98] for charge carrier wave function distortions, our equations (11) and (12) might not be a good fitting tool (however, it does not necessarily mean that in some cases these equations will still be a good fitting tool). Based on all the above, alternative R(T, B) models may be developed for other types of materials.…”
Section: Discussionmentioning
confidence: 99%
“…phonons). However, for materials where the observed T c does not solely depend on the electron-phonon interaction (in particular, in cuprates [51,53,54], pnictides [75][76][77] and nickelates [78,79]), but instead on the thermodynamic fluctuations [58,[80][81][82][83], the presence of pseudogap [84,85], structural disorder [86][87][88][89], system dimensionality [90][91][92][93][94] or other mechanisms [95][96][97][98] for charge carrier wave function distortions, our equations (11) and (12) might not be a good fitting tool (however, it does not necessarily mean that in some cases these equations will still be a good fitting tool). Based on all the above, alternative R(T, B) models may be developed for other types of materials.…”
Section: Discussionmentioning
confidence: 99%