Crystalline electric field excitations in the quantum spin liquid candidate NaYbSe2

Zheng Zhang, Xiaoli Ma, Jianshu Li, Guohua Wang, D. T. Adroja, T. P. Perring, Weiwei Liu, Feng Jin, Jianting Ji, Yimeng Wang, Yoshitomo Kamiya, Xiaoqun Wang, Jie Ma, and Qingming Zhang
Phys. Rev. B 103, 035144 – Published 27 January 2021
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Abstract

By employing inelastic neutron scattering (INS) and Raman scattering (RS) experiments, we comprehensively investigate crystalline electric field (CEF) excitations in NaYbSe2, a new quantum spin liquid candidate that belongs to a large family of triangular-lattice rare-earth chalcogenides with a high-symmetry structure and negligible structural, spin, and charge disordering effects. We can identify CEF excitations at 15.8, 24.3, and 30.5 meV at 5 K. The selected cuts of the INS spectra are well reproduced with a large anisotropy of gab = 2.9 and gc = 1. The CEF excitations are further confirmed by our calculations based on the point charge model. Interestingly, NaYbSe2 exhibits an unusual shift of CEF levels to higher energies with increasing temperatures. Further, the Raman mode close to the first CEF excitation shows an anomalously large softening with decreasing temperatures. The absence of these anomalies in the nonmagnetic isostructural material NaLuSe2 allows us to argue that NaYbSe2 incorporates an unusually strong CEF-phonon resonancelike coupling not reported in any of the triangular-lattice rare-earth chalcogenides. The determination of the CEF excitations suggests the validity of the picture of an effective spin 1/2 at low temperatures.

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  • Received 20 February 2020
  • Revised 10 July 2020
  • Accepted 5 January 2021

DOI:https://doi.org/10.1103/PhysRevB.103.035144

©2021 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

Zheng Zhang1,2, Xiaoli Ma2, Jianshu Li1,2, Guohua Wang3, D. T. Adroja4,5, T. P. Perring4, Weiwei Liu1,2, Feng Jin2, Jianting Ji2, Yimeng Wang1,2, Yoshitomo Kamiya3, Xiaoqun Wang3, Jie Ma3,*, and Qingming Zhang6,2,†

  • 1Department of Physics, Renmin University of China, Beijing 100872, China
  • 2Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China
  • 3Key Laboratory of Artificial Structures and Quantum Control of MOE, Shenyang National Laboratory for Materials Science, Shenyang 110016, China and School of Physics and Astronomy, Tsung-Dao Lee Institute, Shanghai Jiao Tong University, Shanghai 200240, China
  • 4ISIS Neutron and Muon Facility, SCFT Rutherford Appleton Laboratory, Chilton, Didcot Oxon OX11 0QX, United Kingdom
  • 5Highly Correlated Matter Research Group, Physics Department, University of Johannesburg, P.O. Box 524, Auckland Park 2006, South Africa
  • 6School of Physical Science and Technology, Lanzhou University, Lanzhou 730000, China

  • *jma3@sjtu.edu.cn
  • qmzhang@ruc.edu.cn

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Issue

Vol. 103, Iss. 3 — 15 January 2021

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