TY - JOUR
T1 - Interlayer tunneling spectroscopy and doping-dependent energy-gap structure of the trilayer superconductor Bi2Sr2Ca2Cu3O10+δ
AU - Yamada, Yoshiharu
AU - Anagawa, Kenkichi
AU - Shibauchi, Takasada
AU - Fujii, Takenori
AU - Watanabe, Takao
AU - Matsuda, Azusa
AU - Suzuki, Minoru
PY - 2003/8/1
Y1 - 2003/8/1
N2 - The superconducting gap, the pseudogap, and their doping and temperature dependences have been measured by the short-pulse interlayer tunneling spectroscopy for the CuO2 triple-layer high-Tc superconducting Bi2Sr2Ca2Cu3O10+δ system. It is found for a nearly optimally doped sample that the superconducting gap magnitude is ≈80 meV and the pseudogap is ≈120 meV, the values of which are slightly larger than those for CuO2 double-layer system. Both gap magnitudes show a clear tendency to decrease with increasing doping. In an underdoped sample, a clear dip-and-hump structure is observed, which declines with increasing doping and tends to diminish in overdoped samples. The relationship between unchanged Tc and decreasing superconducting gap in the overdoped region is discussed in terms of the proximity effect applied to the inequivalent doping model. We also discuss the dip-and-hump structure in comparison with other spectroscopic results. Finally, we argue an important implication of the increasing maximum Josephson current and the decreasing superconducting gap magnitude, both with increasing doping.
AB - The superconducting gap, the pseudogap, and their doping and temperature dependences have been measured by the short-pulse interlayer tunneling spectroscopy for the CuO2 triple-layer high-Tc superconducting Bi2Sr2Ca2Cu3O10+δ system. It is found for a nearly optimally doped sample that the superconducting gap magnitude is ≈80 meV and the pseudogap is ≈120 meV, the values of which are slightly larger than those for CuO2 double-layer system. Both gap magnitudes show a clear tendency to decrease with increasing doping. In an underdoped sample, a clear dip-and-hump structure is observed, which declines with increasing doping and tends to diminish in overdoped samples. The relationship between unchanged Tc and decreasing superconducting gap in the overdoped region is discussed in terms of the proximity effect applied to the inequivalent doping model. We also discuss the dip-and-hump structure in comparison with other spectroscopic results. Finally, we argue an important implication of the increasing maximum Josephson current and the decreasing superconducting gap magnitude, both with increasing doping.
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U2 - 10.1103/PhysRevB.68.054533
DO - 10.1103/PhysRevB.68.054533
M3 - Article
AN - SCOPUS:0141483448
SN - 1098-0121
VL - 68
JO - Physical Review B - Condensed Matter and Materials Physics
JF - Physical Review B - Condensed Matter and Materials Physics
IS - 5
ER -