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Fulde–Ferrell–Larkin–Ovchinnikov State in Quasi-One-Dimensional Systems: Correlation between Fermi-Surface Distortion and Optimal In-Plane Magnetic-Field Direction

https://hiroshima.repo.nii.ac.jp/records/2007617
https://hiroshima.repo.nii.ac.jp/records/2007617
20684359-ff51-4930-b1b9-75a2665c1354
名前 / ファイル ライセンス アクション
JPSJ_89_024708.pdf JPSJ_89_024708.pdf (885.2 KB)
Item type デフォルトアイテムタイプ_(フル)(1)
公開日 2023-03-18
タイトル
タイトル Fulde–Ferrell–Larkin–Ovchinnikov State in Quasi-One-Dimensional Systems: Correlation between Fermi-Surface Distortion and Optimal In-Plane Magnetic-Field Direction
言語 en
作成者 Itahashi, Katsumi

× Itahashi, Katsumi

en Itahashi, Katsumi

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Shimahara, Hiroshi

× Shimahara, Hiroshi

en Shimahara, Hiroshi

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アクセス権
アクセス権 open access
アクセス権URI http://purl.org/coar/access_right/c_abf2
権利情報
権利情報 Copyright (c) 2020 The Physical Society of Japan
権利情報
権利情報 This is not the published version. Please cite only the published version. この論文は出版社版ではありません。引用の際には出版社版をご確認、ご利用ください。
内容記述
内容記述 The Fulde–Ferrell–Larkin–Ovchinnikov (FFLO) state is systematically examined in a generic model of quasi-one-dimensional (Q1D) type-II superconductors that has six hopping integrals of electrons as model parameters. For a magnetic field parallel to the conductive layers, the upper critical field Hc2 is strongly enhanced by the FFLO state at low temperatures and sensitively depends on the angle ϕ between the in-plane magnetic field and the highly conductive chain (the crystal a-axis). As a result, Hc2 exhibits sharp peaks at the optimal angles ϕ = ±ϕ0. Since the optimal angle ϕ0 strongly depends on the structure of the Fermi surface, we examine their correlation, searching for an intuitive method to find ϕ0 from the shape of the Fermi surface. For this purpose, we define quantities that quantify the warp of each sheet (kx > 0 or kx < 0) of the Q1D open Fermi surface and the shear distortion between the two sheets. We estimate the optimal angles for numbers of the parameter sets chosen systematically from a large area of the parameter space. It is found that in most cases, the optimal direction of the in-plane magnetic field tends to be roughly parallel to the a-axis. This result, together with the fact that the orbital pair-breaking effect is weakest for ϕ = 0, implies that the FFLO state is most stabilized for a small ϕ. However, when the warp is small while the shear distortion is moderate, the FFLO state can be maximally stabilized for any in-plane magnetic-field direction except for the directions between the b- and b′-axes, where the b′-axis is perpendicular to the a-axis. The phase diagrams of the optimal angle and the upper critical field at zero temperature are also presented. A jump of the optimal angle ϕ0 when the pressure varies is predicted.
言語 en
出版者
出版者 The Physical Society of Japan
言語
言語 eng
資源タイプ
資源タイプ識別子 http://purl.org/coar/resource_type/c_6501
資源タイプ journal article
出版タイプ
出版タイプ AO
出版タイプResource http://purl.org/coar/version/c_b1a7d7d4d402bcce
関連情報
識別子タイプ DOI
関連識別子 10.7566/JPSJ.89.024708
関連情報
識別子タイプ DOI
関連識別子 https://doi.org/10.7566/JPSJ.89.024708
収録物識別子
収録物識別子タイプ ISSN
収録物識別子 0031-9015
開始ページ
開始ページ 024708-1
書誌情報 Journal of the Physical Society of Japan
Journal of the Physical Society of Japan

巻 89, p. 024708-1-024708-8, 発行日 2020-01-29
旧ID 51553
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