Elucidation of Spin-Correlations, Fermi Surface and Pseudogap in a Copper Oxide Superconductor

Author:

Kamimura Hiroshi1,Araidai Masaaki2ORCID,Ishida Kunio3,Matsuno Shunichi4,Sakata Hideaki5,Sasaoka Kenji6,Shiraishi Kenji2,Sugino Osamu7ORCID,Tsai Jaw-Shen58,Yamada Kazuyoshi9

Affiliation:

1. Tokyo University of Science, 1-3 Kagurazaka, Shinjuku-ku, Tokyo 162-8601, Japan

2. Institute of Materials and Systems for Sustainability, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8601, Japan

3. Graduate School of Engineering, Utsunomiya University, Utsunomiya 321-8585, Japan

4. School of Marine Science and Technology, Tokai University, Shimizu 424-8610, Japan

5. Graduate School of Science, Faculty of Science, Tokyo University of Science, 1-3 Kagurazaka, Shinjuku-ku, Tokyo 162-8601, Japan

6. Water Frontier Research Center, Research Institute for Science and Technology, Tokyo University of Science, 1-3 Kagurazaka, Shinjuku-ku, Tokyo 162-8601, Japan

7. Institute of Solid State Physics, University of Tokyo, 5-1-5 Kashiwanoha, Kashiwa, Chiba 277-8581, Japan

8. RIKEN Center for Quantum Computing (RQC), Wako, Saitama 351-0198, Japan

9. Post KEK, 1-1 Oho, Tsukuba, Ibaraki 305-0801, Japan

Abstract

First-principles calculations for underdoped La2−xSrxCuO4 (LSCO) have revealed a Fermi surface consisting of spin-triplet (KS) particles at the antinodal Fermi-pockets and spin-singlet (SS) particles at the nodal Fermi-arcs in the presence of AF local order. By performing a unique method of calculating the electronic-spin state of overdoped LSCO and by measurement of the spin-correlation length by neutron inelastic scattering, the origin of the phase-diagram, including the pseudogap phase in the high temperature superconductor, Sr-doped copper-oxide LSCO, has been elucidated. We have theoretically solved the long-term problem as to why the angle-resolved photoemission spectroscopy (ARPES) has not been able to observe Fermi pockets in the Fermi surface of LSCO. As a result, we show that the pseudogap region is bounded below the characteristic temperature T*(x) and above the superconducting transition temperature Tc(x) in the T vs. x phase diagram, where both the AF order and the KS particles in the Fermi pockets vanish at T*(x), whilst KS particles contribute to d-wave superconductivity below Tc. We also show that the relationship T*(xc) = Tc(xc) holds at xc = 0.30, which is consistent with ARPES experiments. At T*(x), a phase transition occurs from the pseudogap phase to an unusual metallic phase in which only the SS particles exist.

Funder

Tokyo University of Science

Publisher

MDPI AG

Subject

Condensed Matter Physics,Electronic, Optical and Magnetic Materials

Reference38 articles.

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3. Kamimura, H., Araidai, M., Ishida, K., Matsuno, S., Sakata, H., Shiraishi, K., Sugino, O., and Tsai, J.S. (2020). First-Principles Calculation of copper oxide superconductors that supports the Kamimura-Suwa model. Condens. Matter, 5.

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5. Singlet and triplet hole-doped configuration in La2Cu0.5Li0.5O4;Anisimov;Phys. Rev. B,1997

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