TY - JOUR
T1 - Flux creep after field trapping in YBa2Cu3Ox foams
AU - Koblischka, M. R.
AU - Pavan Kumar Naik, S.
AU - Koblischka-Veneva, A.
AU - Gokhfeld, D.
AU - Murakami, M.
N1 - Publisher Copyright:
© 2020 IOP Publishing Ltd.
PY - 2020
Y1 - 2020
N2 - The time-dependence of the field distribution on the surface of YBa2Cu3Ox (YBCO) foam samples after field trapping is analysed. The foam samples were magnetised using a bulk permanent magnet at 77 K, and the trapped fields (TFs) were recorded with a scanning Hall probe 1 mm above the sample surface. Besides a large TF peak, several small peaks are observed. The time dependence of the local fields of these peaks and of the large peak are clearly different, which points to a different origin. In this way, the time-dependent TF measurements reveal important information about the current flow in the foam samples. A non-logarithmic relaxation process takes place in the foam samples. Furthermore, we compare these results with classic creep measurements performed on an individual foam strut removed from the bulk. The creep rate for the TF distribution is found to be ∼8%, whereas the creep rate of the foam strut is about 4% in a large temperature and field range (20-60 K, 0-2 T).
AB - The time-dependence of the field distribution on the surface of YBa2Cu3Ox (YBCO) foam samples after field trapping is analysed. The foam samples were magnetised using a bulk permanent magnet at 77 K, and the trapped fields (TFs) were recorded with a scanning Hall probe 1 mm above the sample surface. Besides a large TF peak, several small peaks are observed. The time dependence of the local fields of these peaks and of the large peak are clearly different, which points to a different origin. In this way, the time-dependent TF measurements reveal important information about the current flow in the foam samples. A non-logarithmic relaxation process takes place in the foam samples. Furthermore, we compare these results with classic creep measurements performed on an individual foam strut removed from the bulk. The creep rate for the TF distribution is found to be ∼8%, whereas the creep rate of the foam strut is about 4% in a large temperature and field range (20-60 K, 0-2 T).
KW - YBCO
KW - flux creep
KW - superconducting foam
KW - trapped fields
UR - http://www.scopus.com/inward/record.url?scp=85082383556&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=85082383556&partnerID=8YFLogxK
U2 - 10.1088/1361-6668/ab72c3
DO - 10.1088/1361-6668/ab72c3
M3 - Article
AN - SCOPUS:85082383556
SN - 0953-2048
VL - 33
JO - Superconductor Science and Technology
JF - Superconductor Science and Technology
IS - 4
M1 - 044008
ER -