2011
DOI: 10.1103/physrevb.84.104528
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Theory and simulations on strong pinning of vortex lines by nanoparticles

Abstract: Pinning of vortex lines by array of nanoparticles embedded inside superconductors became the most efficient practical way to achieve high critical currents. In this situation pinning occurs via trapping of the vortex-line segments and the critical current is determined by the typical length of trapped segment. To verify analytical estimates and develop a quantitative description of strong pinning, we numerically simulated isolated vortex lines driven through array of nanoparticles. We found that the critical f… Show more

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Cited by 66 publications
(78 citation statements)
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“…The NPs are responsible for the increases in the wider angular range and the TBs are more effective near the c axis. The broad dome-shape like increase in μ 0 H irr ( θ )– ε ( θ )μ 0 H irr due to the NPs resembles the increases found in J c in samples with nanosized inclusions, both in YBCO and Fe-based superconductors1026272829. The reason for this dome shape (or inverse anisotropy) is found in the fact that while NPs are randomly dispersed, they are not point defects, thus do not follow the electronic mass anisotropy scaling as point defects do21.…”
Section: Resultssupporting
confidence: 52%
“…The NPs are responsible for the increases in the wider angular range and the TBs are more effective near the c axis. The broad dome-shape like increase in μ 0 H irr ( θ )– ε ( θ )μ 0 H irr due to the NPs resembles the increases found in J c in samples with nanosized inclusions, both in YBCO and Fe-based superconductors1026272829. The reason for this dome shape (or inverse anisotropy) is found in the fact that while NPs are randomly dispersed, they are not point defects, thus do not follow the electronic mass anisotropy scaling as point defects do21.…”
Section: Resultssupporting
confidence: 52%
“…Koshelev et al 39 studied theoretically the effect of an array of nanoparticles on the vortex line pinning and found that the critical current is determined by the length of the trapped segment, leading to L ∝ n . In this model, the critical force grows roughly as n 1/2 .…”
Section: Resultsmentioning
confidence: 99%
“…Several models have been proposed to explain J c (T, H, θ) in cuprate and pnictide superconductors with strong pinning NPs or NRs. 21,24,[50][51][52][53][54][55][56][57][58][59] Although the influence of creep Tuning NP size for enhanced functionality M Miura et al on J c for these superconductors has been known for a long time, 49,60 only a few attempts have been made to link the pinning improvements to J c and S. 60,61 To calculate the temperature, magnetic field and field angle dependence of J c (J c;calc: ), we use J c;calc: T; H; y ð Þ¼ J c0 T; H; y ð Þ1 À Sln t=t 0 ð Þ ð Þ , where t 0 is the effective attempt time, J c0 is the creep-free J c and S is the experimentally obtained flux creep rate.…”
Section: Dramatically Higher J C With Nearly Isotropic Angular Dependmentioning
confidence: 99%