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Gap structure of FeSe determined by angle-resolved specific heat measurements in applied rotating magnetic field

Yue Sun, Shunichiro Kittaka, Shota Nakamura, Toshiro Sakakibara, Koki Irie, Takuya Nomoto, Kazushige Machida, Jingting Chen, and Tsuyoshi Tamegai
Phys. Rev. B 96, 220505(R) – Published 19 December 2017
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Abstract

Quasiparticle excitations in FeSe were studied by means of specific heat (C) measurements on a high-quality single crystal under rotating magnetic fields. The field dependence of C shows three-stage behavior with different slopes, indicating the existence of three gaps (Δ1,Δ2, and Δ3). In the low-temperature and low-field region, the azimuthal angle (ϕ) dependence of C shows a fourfold symmetric oscillation with a sign change. On the other hand, the polar angle (θ) dependence manifests as an anisotropy-inverted twofold symmetry with unusual shoulder behavior. Combining the angle-resolved results and the theoretical calculation, the smaller gap Δ1 is proved to have two vertical-line nodes or gap minima along the kz direction, and is determined to reside on the electron-type ɛ band. Δ2 is found to be related to the electron-type δ band, and is isotropic in the ab plane but largely anisotropic out of the plane. Δ3 residing on the hole-type α band shows a small out-of-plane anisotropy with a strong Pauli paramagnetic effect.

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  • Received 26 June 2017

DOI:https://doi.org/10.1103/PhysRevB.96.220505

©2017 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

Yue Sun1,*, Shunichiro Kittaka1, Shota Nakamura1, Toshiro Sakakibara1, Koki Irie2, Takuya Nomoto3, Kazushige Machida2, Jingting Chen4, and Tsuyoshi Tamegai4

  • 1Institute for Solid State Physics (ISSP), The University of Tokyo, Kashiwa, Chiba 277-8581, Japan
  • 2Department of Physics, Ritsumeikan University, Kusatsu, Shiga 525-8577, Japan
  • 3RIKEN Center for Emergent Matter Science (CEMS), Hirosawa, Wako, Saitama 351-0198, Japan
  • 4Department of Applied Physics, The University of Tokyo, Bunkyo-ku, Tokyo 113-8656, Japan

  • *sunyue@issp.u-tokyo.ac.jp

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Issue

Vol. 96, Iss. 22 — 1 December 2017

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Images

  • Figure 1
    Figure 1

    (a) Definitions of azimuthal (ϕ) and polar (θ) angles with respect to the crystal axes. The Se in the center is on the layer below. (b) Normalized zero-field electronic specific heat Ce/γnT vs T, together with the fit by a three-gap model. (c) Magnetic field dependences of C(H)/T for Hc and Hab at 0.6 K.

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  • Figure 2
    Figure 2

    (a) Azimuthal angle dependence of the specific heat ΔC(ϕ)/T measured under various fields at 0.33 K. ΔC(ϕ)/T is defined as C(ϕ)/TC(45)/T, and each subsequent curve is shifted vertically by 0.2 mJ/molK2. Symbols with black outlines are measured data, and those without are mirrored points to show the symmetry. (b) Polar plot of the ΔC(ϕ)/T at 0.33 K under 0.8 T. (c) ΔC(ϕ)/T measured under 0.8 T at 0.33, 0.60, and 2.1 K. Each subsequent curve is shifted by 0.2 mJ/molK2. (d) In-plane schematic view of the atomic arrangement and gap structure of Δɛ [19] in domains A and B sandwiching a TB. Schematic gap functions of Δɛ in domains (e) A and (f) B, and (g) their superpositions.

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  • Figure 3
    Figure 3

    Polar angle dependence of the specific heat ΔC(θ)/T measured under fields (a) below and (b) above 1 T at 0.33 K. ΔC(θ)/T is defined as C(θ)/TC(90)/T, and each subsequent curve is shifted vertically by 2 mJ/molK2. Symbols outlined in black are the measured data; the others are mirrored points to show the symmetry more clearly. (c) Calculated Fermi surface cross section for the ɛ band along the kz direction. (d) Schematic gap structure for the ɛ band in 3D. (e) Calculated results of the θ dependence of the zero-energy DOS, N(E=0), in magnetic fields normalized by Hc2.

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