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Development of Ferromagnetic Fluctuations in Heavily Overdoped (Bi,Pb)_{2}Sr_{2}CuO_{6+δ} Copper Oxides

We demonstrate the presence of ferromagnetic (FM) fluctuations in the superconducting and nonsuperconducting heavily overdoped regimes of high-temperature superconducting copper oxides, using (Bi,Pb)_{2}Sr_{2}CuO_{6+δ} (Bi-2201) single crystals. Magnetization curves exhibit a tendency to be saturate...

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Published in:Physical review letters 2018-08, Vol.121 (5), p.057002-057002
Main Authors: Kurashima, Koshi, Adachi, Tadashi, Suzuki, Kensuke M, Fukunaga, Yasushi, Kawamata, Takayuki, Noji, Takashi, Miyasaka, Hitoshi, Watanabe, Isao, Miyazaki, Masanori, Koda, Akihiro, Kadono, Ryosuke, Koike, Yoji
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container_title Physical review letters
container_volume 121
creator Kurashima, Koshi
Adachi, Tadashi
Suzuki, Kensuke M
Fukunaga, Yasushi
Kawamata, Takayuki
Noji, Takashi
Miyasaka, Hitoshi
Watanabe, Isao
Miyazaki, Masanori
Koda, Akihiro
Kadono, Ryosuke
Koike, Yoji
description We demonstrate the presence of ferromagnetic (FM) fluctuations in the superconducting and nonsuperconducting heavily overdoped regimes of high-temperature superconducting copper oxides, using (Bi,Pb)_{2}Sr_{2}CuO_{6+δ} (Bi-2201) single crystals. Magnetization curves exhibit a tendency to be saturated in high magnetic fields at low temperatures in the heavily overdoped crystals, which is probably a precursor phenomenon of a FM transition at a lower temperature. Muon spin relaxation detects the enhancement of spin fluctuations at high temperatures below 200 K. Correspondingly, the ab-plane resistivity follows a 4/3 power law in a wide temperature range, which is characteristic of metals with two-dimensional FM fluctuations due to itinerant electrons. As the Wilson ratio evidences the enhancement of spin fluctuations with hole doping in the heavily overdoped regime, it is concluded that two-dimensional FM fluctuations reside in the heavily overdoped Bi-2201 cuprates, which is probably related to the decrease in the superconducting transition temperature in the heavily overdoped cuprates.
doi_str_mv 10.1103/PhysRevLett.121.057002
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