TY - JOUR
T1 - Tunneling break-junction spectroscopy on the superconductor NdFeAs(O 0.9F0.1)
AU - Ekino, Toshikazu
AU - Sugimoto, Akira
AU - Okabe, Hirotaka
AU - Shohara, Kazuhiro
AU - Ukita, Ryuichi
AU - Akimitsu, Jun
AU - Gabovich, Alexander M.
N1 - Funding Information:
This work was supported by a Grant-in-Aid for Scientific Research (Nos. 19540370, 19105006, 19014016 ) of Japan Society of Promotion of Science . AMG highly appreciates FY2007 fellowship no. S-07042 Granted by the Japan Society for the Promotion of Science as well as the support given in 2009 by the Visitors Program of the Max Planck Institute for the Physics of Complex Systems (Dresden, Germany).
PY - 2010/12
Y1 - 2010/12
N2 - Tunnel break-junction method has been adopted to study polycrystalline samples of iron-oxypnictide superconductor NdFeAs(O0.9F 0.1) with Tc=48K. Measurements were carried out at 4.2 K. Break-junction (BJ) conductance versus voltage curves showed gap-edge peaks with the peak-to-peak distances Vp-p=4Δ/e=28-40mV at 4.2 K, where 2Δ(T) is the superconducting energy gap, e>0 is the elementary charge. This yields 2Δ(0)=14-20meV, so that the gap ratio 2Δ(0)/kBTc is about 4.1±0.7,kB being the Boltzmann constant. This ratio implies strong-coupling superconductivity in the framework of Bardeen-Cooper-Schrieffer theory, being, however, much smaller than that for high-Tc copper oxides. This suggests a significant difference in the pairing mechanism between those classes of materials.
AB - Tunnel break-junction method has been adopted to study polycrystalline samples of iron-oxypnictide superconductor NdFeAs(O0.9F 0.1) with Tc=48K. Measurements were carried out at 4.2 K. Break-junction (BJ) conductance versus voltage curves showed gap-edge peaks with the peak-to-peak distances Vp-p=4Δ/e=28-40mV at 4.2 K, where 2Δ(T) is the superconducting energy gap, e>0 is the elementary charge. This yields 2Δ(0)=14-20meV, so that the gap ratio 2Δ(0)/kBTc is about 4.1±0.7,kB being the Boltzmann constant. This ratio implies strong-coupling superconductivity in the framework of Bardeen-Cooper-Schrieffer theory, being, however, much smaller than that for high-Tc copper oxides. This suggests a significant difference in the pairing mechanism between those classes of materials.
KW - Break-junction
KW - Energy gap
KW - Iron-oxypnictide superconductors
KW - Tunneling
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U2 - 10.1016/j.physc.2009.10.079
DO - 10.1016/j.physc.2009.10.079
M3 - Article
AN - SCOPUS:78649690498
SN - 0921-4534
VL - 470
SP - S358-S359
JO - Physica C: Superconductivity and its Applications
JF - Physica C: Superconductivity and its Applications
IS - SUPPL.1
ER -