TY - JOUR
T1 - Enhancement of the superconducting transition temperature by the Sr-substitution for Ba in (Yb,Ca)Ba2Cu3O6
AU - Nakagawa, Kohei
AU - Sumino, Yoshiki
AU - Kim, Keon
AU - Noji, Takashi
AU - Kawamata, Takayuki
AU - Koike, Yoji
AU - Kato, Masatsune
N1 - Funding Information:
This work was supported by JSPS KAKENHI grant number JP15K06433 .
Publisher Copyright:
© 2019
PY - 2019/9/15
Y1 - 2019/9/15
N2 - We have investigated the effect of the Sr-substitution for Ba on the superconductivity in Yb0.6Ca0.4Ba2- ySryCu3O6 without Ochain forming the so-called Cu(1)O chain in the blocking layer. It has been found that Tc increases with increasing y even though no holes are doped through the Sr2+-substitution for Ba2+. The increase in Tc is because holes doped by the Ca-substitution for Yb are more likely supplied to the superconducting Cu(2)O2 plane than the blocking layer of Cu(1) owing to the contraction of the Cu(2)O2 plane through the substitution of smaller Sr2+ for larger Ba2+. The highest Tc onset = 73 K observed for y(Sr) = 0.6 is greatly higher than the previous record of Tc onset = 50 K in (RE,Ca)Ba2Cu3O6 (RE: rare-earth element). The reason why it is lower than ∼90 K for REBa2Cu3O7 is the low hole-concentration in the Cu(2)O2 plane.
AB - We have investigated the effect of the Sr-substitution for Ba on the superconductivity in Yb0.6Ca0.4Ba2- ySryCu3O6 without Ochain forming the so-called Cu(1)O chain in the blocking layer. It has been found that Tc increases with increasing y even though no holes are doped through the Sr2+-substitution for Ba2+. The increase in Tc is because holes doped by the Ca-substitution for Yb are more likely supplied to the superconducting Cu(2)O2 plane than the blocking layer of Cu(1) owing to the contraction of the Cu(2)O2 plane through the substitution of smaller Sr2+ for larger Ba2+. The highest Tc onset = 73 K observed for y(Sr) = 0.6 is greatly higher than the previous record of Tc onset = 50 K in (RE,Ca)Ba2Cu3O6 (RE: rare-earth element). The reason why it is lower than ∼90 K for REBa2Cu3O7 is the low hole-concentration in the Cu(2)O2 plane.
KW - Cuprate superconductor
KW - Elemental substitution
KW - Hole concentration
KW - RE-123 structure
KW - Superconducting transition temperature
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U2 - 10.1016/j.physc.2019.06.001
DO - 10.1016/j.physc.2019.06.001
M3 - Article
AN - SCOPUS:85066989645
SN - 0921-4534
VL - 564
SP - 38
EP - 41
JO - Physica C: Superconductivity and its Applications
JF - Physica C: Superconductivity and its Applications
ER -