TY - JOUR
T1 - Doping dependencies of onset temperatures for the pseudogap and superconductive fluctuation in Bi2Sr2CaCu2O8+δ, studied from both in-plane and out-of-plane magnetoresistance measurements
AU - Usui, Tomohiro
AU - Fujiwara, Daiki
AU - Adachi, Shintaro
AU - Kudo, Hironobu
AU - Murata, Kosuke
AU - Kushibiki, Haruki
AU - Watanabe, Takao
AU - Kudo, Kazutaka
AU - Nishizaki, Terukazu
AU - Kobayashi, Norio
AU - Kimura, Shojiro
AU - Yamada, Kazuyoshi
AU - Naito, Tomoyuki
AU - Noji, Takashi
AU - Koike, Yoji
N1 - Publisher Copyright:
© 2014 The Physical Society of Japan.
PY - 2014/6/15
Y1 - 2014/6/15
N2 - To investigate the relationship between the pseudogap and superconductivity, we measured both the in-plane (ρab) and out-of-plane (ρc) resistivity for oxygen-controlled Bi2Sr2CaCu2O8+δ single crystals subject to magnetic fields (parallel to the c-axis) of up to 17.5 T. The onset temperature for the superconductive fluctuation, Tscf, is determined by the large positive in-plane magnetoresistance (MR) and negative out-of-plane MR observed near Tc, whereas the pseudogap opening temperature T is determined by the semiconductive upturn of the zero-field ρc. Tscf was found to scale roughly as Tc, with a decreasing temperature interval between them upon doping. On the other hand, T starts out much higher than Tscf but decreases monotonically upon doping; finally, at a heavily overdoped state, it is not observed above Tscf. These results imply that the pseudogap is not a simple precursor of superconductivity, but that further study is needed to determine whether or not T exists below Tscf in the heavily overdoped state.
AB - To investigate the relationship between the pseudogap and superconductivity, we measured both the in-plane (ρab) and out-of-plane (ρc) resistivity for oxygen-controlled Bi2Sr2CaCu2O8+δ single crystals subject to magnetic fields (parallel to the c-axis) of up to 17.5 T. The onset temperature for the superconductive fluctuation, Tscf, is determined by the large positive in-plane magnetoresistance (MR) and negative out-of-plane MR observed near Tc, whereas the pseudogap opening temperature T is determined by the semiconductive upturn of the zero-field ρc. Tscf was found to scale roughly as Tc, with a decreasing temperature interval between them upon doping. On the other hand, T starts out much higher than Tscf but decreases monotonically upon doping; finally, at a heavily overdoped state, it is not observed above Tscf. These results imply that the pseudogap is not a simple precursor of superconductivity, but that further study is needed to determine whether or not T exists below Tscf in the heavily overdoped state.
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U2 - 10.7566/JPSJ.83.064713
DO - 10.7566/JPSJ.83.064713
M3 - Article
AN - SCOPUS:84924898351
SN - 0031-9015
VL - 83
JO - Journal of the Physical Society of Japan
JF - Journal of the Physical Society of Japan
IS - 6
M1 - 064713
ER -