SLIDE 9 Analysis: Jc(q) at 7 T
- How to explain and predict the behaviour with temperature?
- At higher temperature (65K) we have a large uniform component and 2
c-axis components
– Must be 2 defect populations broadening the c-axis pinning
- Stacking faults
- Intrinsic ab-plane pinning? Point defects?
– No ab-plane peak as stacking faults density not high enough
– Always have a large isotropic averaging (green component)
- At low T – dominant intrinsic ab-plane pinning gives a peaked
distribution
- For prediction of Jc need a map of components in (B,T) space
– R Knibbe et al, SuST 29 (6), 065006 9
30 60 90 120 150 180 210 500 1000 1500 2000 2500
Ic(A/cm) Angle(°) 20K 7T 6E11 ions G = 0.194
30 60 90 120 150 180 210 20 40 60 80 100
Ic(A/cm) Angle(°) 65 K 7 T 6E11 ions 1 = 1.22, 2 = 2.82
30 60 90 120 150 180 210 500 1000 1500
Ic(A/cm) Angle(°) 30 K 7 T 6E11 ions G = 0.098
T
IEEE CSC & ESAS SUPERCONDUCTIVITY NEWS FORUM (global edition), February 2020. Presentation AT-5 given at ACASC/Asian-ICMC, 6-9 January 2020, Okinawa, Japan.