TY - JOUR
T1 - STM/STS study of the superconducting gap in SmFeAsO1-xFx
AU - Kawashima, Yuki
AU - Ichimura, Koichi
AU - Katono, Kazuhiro
AU - Kurosawa, Tohru
AU - Oda, Migaku
AU - Tanda, Satoshi
AU - Kamihara, Yoichi
AU - Hosono, Hideo
N1 - Funding Information:
This work was supported by the 21COE program on “Topological Science and Technology” of the Ministry of Education, Culture, Sport, Science and Technology of Japan. This work was partially supported by the Asahi Glass Foundation, and the Japan Society for Promotion of Science (JSPS) KAKENHI Grant no. 26400337 .
Publisher Copyright:
© 2014 Published by Elsevier Ltd.
PY - 2015/2
Y1 - 2015/2
N2 - We report an electron tunneling study of SmFeAsO1-xFx in the low doping region (x=0, 0.045, 0.046, 0.069) by low temperature UHV-STM/STS. Superconducting gaps are observed for each superconducting sample x=0.045 (Tc=12.9 K), x=0.046 (Tc=32.9 K) and x=0.069 (Tc=46.9 K). We obtained corresponding superconducting gap size of ΔSC=9.5±0.5meV, 9.75±0.25 meV and 11±1 meV. While Tc increases, ΔSC is kept the same. This suggests that the effective attractive interaction is the same and that there is some mechanism that suppresses the superconductivity in the low doping region. On the other hand, similar gap structures were found in a non-superconducting sample with x=0 at 7.8 K. The obtained gap size was ΔN=8.5±1.5meV, which is almost the same as the superconducting gap in the superconducting samples (x=0.045, 0.046, 0.069).
AB - We report an electron tunneling study of SmFeAsO1-xFx in the low doping region (x=0, 0.045, 0.046, 0.069) by low temperature UHV-STM/STS. Superconducting gaps are observed for each superconducting sample x=0.045 (Tc=12.9 K), x=0.046 (Tc=32.9 K) and x=0.069 (Tc=46.9 K). We obtained corresponding superconducting gap size of ΔSC=9.5±0.5meV, 9.75±0.25 meV and 11±1 meV. While Tc increases, ΔSC is kept the same. This suggests that the effective attractive interaction is the same and that there is some mechanism that suppresses the superconductivity in the low doping region. On the other hand, similar gap structures were found in a non-superconducting sample with x=0 at 7.8 K. The obtained gap size was ΔN=8.5±1.5meV, which is almost the same as the superconducting gap in the superconducting samples (x=0.045, 0.046, 0.069).
KW - A. Iron-based superconductor
KW - D. Superconducting gap
KW - E. STM
UR - http://www.scopus.com/inward/record.url?scp=84920091984&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=84920091984&partnerID=8YFLogxK
U2 - 10.1016/j.ssc.2014.12.003
DO - 10.1016/j.ssc.2014.12.003
M3 - Article
AN - SCOPUS:84920091984
SN - 0038-1098
VL - 204
SP - 33
EP - 36
JO - Solid State Communications
JF - Solid State Communications
ER -