TY - JOUR
T1 - Unscaling superconducting parameters with Tc for Bi-2212 and Bi-2223
T2 - A magnetotransport study in the superconductive fluctuation regime
AU - Adachi, Shintaro
AU - Usui, Tomohiro
AU - Ito, Yasuhito
AU - Kudo, Hironobu
AU - Kushibiki, Haruki
AU - Murata, Kosuke
AU - Watanabe, Takao
AU - Kudo, Kazutaka
AU - Nishizaki, Terukazu
AU - Kobayashi, Norio
AU - Kimura, Shojiro
AU - Fujita, Masaki
AU - Yamada, Kazuyoshi
AU - Noji, Takashi
AU - Koike, Yoji
AU - Fujii, Takenori
N1 - Publisher Copyright:
© 2015 The Physical Society of Japan.
PY - 2015/2/15
Y1 - 2015/2/15
N2 - To investigate the origin of the enhanced Tc (≈ 110 K) of the trilayer cuprate superconductor Bi2Sr2Ca2Cu3O10+δ (Bi-2223), we have performed systematic magnetoresistance (MR) measurements on this superconductor, as well as on the bilayer superconductor, Bi2Sr2CaCu2O8+δ (Bi-2212). The in-plane coherence length, ξab, and the specific-heat jump, ΔC, have been estimated using the theory of renormalized superconductive fluctuations, and the doping dependence of these parameters has been qualitatively explained using the Fermi arc approach. A detailed comparison of the superconducting parameters with Tc for these compounds suggests that an additional superconducting condensation energy exists, due to an increase in the number of stacking CuO2 planes in a unit cell.
AB - To investigate the origin of the enhanced Tc (≈ 110 K) of the trilayer cuprate superconductor Bi2Sr2Ca2Cu3O10+δ (Bi-2223), we have performed systematic magnetoresistance (MR) measurements on this superconductor, as well as on the bilayer superconductor, Bi2Sr2CaCu2O8+δ (Bi-2212). The in-plane coherence length, ξab, and the specific-heat jump, ΔC, have been estimated using the theory of renormalized superconductive fluctuations, and the doping dependence of these parameters has been qualitatively explained using the Fermi arc approach. A detailed comparison of the superconducting parameters with Tc for these compounds suggests that an additional superconducting condensation energy exists, due to an increase in the number of stacking CuO2 planes in a unit cell.
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U2 - 10.7566/JPSJ.84.024706
DO - 10.7566/JPSJ.84.024706
M3 - Article
AN - SCOPUS:84924943125
SN - 0031-9015
VL - 84
JO - Journal of the Physical Society of Japan
JF - Journal of the Physical Society of Japan
IS - 2
M1 - 024706
ER -