Mechanism of plain s-wave superconductivity in heavy fermion compounds near magnetic criticality: Impact of vertex corrections for gap equation
ORAL
Abstract
We study the orbital-fluctuation-mediated pairing mechanism in heavy fermion systems, motivated by the recent experimental repots of emerging the plane s-wave state without sign-reversal in CeCu2Si2. For this purpose,
we study the recently developed improved gap equation on the basis of the multiorbital periodic Anderson model in the presence of strong spin-orbit interaction (SOI). We take account of the vertex correction for the bare Coulomb interaction (U-VC), which represents the higher-order many-body-effects beyond the Migdal-Eliashberg approximation [1]. We find that the plain s-wave state is realized against the strong Coulomb interaction since the orbital-fluctuation-mediated attractive interaction, driven by the VCs and the e-ph interactions, is strongly enhanced by the U-VC. Near the magnetic criticality, the U-VC becomes significant due to the Aslamazov-Larkin process, which is analogous to the Kugel-Khomskii orbital-spin coupling term in the strong-coupling model. We conclude that the plain s-wave state is realized in multiorbital heavy-fermion systems since the strong SOI magnifies the U-VC in 4f electron systems. [1] R.tazai, Y. Yamakawa, and H. Kontani, J. Phys, Soc. Jpn. 86, 073703 (2017).
we study the recently developed improved gap equation on the basis of the multiorbital periodic Anderson model in the presence of strong spin-orbit interaction (SOI). We take account of the vertex correction for the bare Coulomb interaction (U-VC), which represents the higher-order many-body-effects beyond the Migdal-Eliashberg approximation [1]. We find that the plain s-wave state is realized against the strong Coulomb interaction since the orbital-fluctuation-mediated attractive interaction, driven by the VCs and the e-ph interactions, is strongly enhanced by the U-VC. Near the magnetic criticality, the U-VC becomes significant due to the Aslamazov-Larkin process, which is analogous to the Kugel-Khomskii orbital-spin coupling term in the strong-coupling model. We conclude that the plain s-wave state is realized in multiorbital heavy-fermion systems since the strong SOI magnifies the U-VC in 4f electron systems. [1] R.tazai, Y. Yamakawa, and H. Kontani, J. Phys, Soc. Jpn. 86, 073703 (2017).
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Presenters
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Rina Tazai
Department of Physics, Nagoya university
Authors
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Rina Tazai
Department of Physics, Nagoya university
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Youichi Yamakawa
IAR, Nagoya Univ., Department of Physics, Nagoya university, Nagoya Univ, Department of Physics, Nagoya University, Physics, Nagoya University, Department of Physics, Nagoya Univ
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Hiroshi Kontani
Department of Physics, Nagoya university, Nagoya Univ, Department of Physics, Nagoya University, Department of Physics, Nagoya Univ