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Abstract
A recent focus of quantum spin liquid (QSL) studies is how disorder/randomness in a QSL candidate affects its true magnetic ground state. The ultimate question is whether the QSL survives disorder or the disorder leads to a “spin-liquid-like” state, such as the proposed random-singlet (RS) state. Since disorder is a standard feature of most QSL candidates, this question represents a major challenge for QSL candidates. YbMgGaO4, a triangular lattice antiferromagnet with effective spin-1/2 Yb3+ions, is an ideal system to address this question, since it shows no long-range magnetic ordering with Mg/Ga site disorder. Despite the intensive study, it remains unresolved as to whether YbMgGaO4 is a QSL or in the RS state. Here, through ultralow-temperature thermal conductivity and magnetic torque measurements, plus specific heat and DC magnetization data, we observed a residual κ0/T term and series of quantum spin state transitions in the zero temperature limit for YbMgGaO4. These observations strongly suggest that a QSL state with itinerant excitations and quantum spin fluctuations survives disorder in YbMgGaO4.
It remains an open question as to whether the quantum spin liquid state survives material disorder, or is replaced by some spin-liquid like state. Here, Rao et al succeed in resolving a resolving a κ0/T residual in the thermal conductivity of YbMgGaO4 strongly suggesting the survival of the quantum spin liquid state.
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1 University of Science and Technology of China, Hefei National Laboratory for Physical Sciences at Microscale, Department of Physics, and Key Laboratory of Strongly-Coupled Quantum Matter Physics (CAS), Hefei, People’s Republic of China (GRID:grid.59053.3a) (ISNI:0000000121679639)
2 University of Tennessee, Department of Physics and Astronomy, Knoxville, USA (GRID:grid.411461.7) (ISNI:0000 0001 2315 1184)
3 University of Science and Technology of China, School of Physical Sciences, Hefei, People’s Republic of China (GRID:grid.59053.3a) (ISNI:0000000121679639)
4 Florida State University, National High Magnetic Field Laboratory, Tallahassee, USA (GRID:grid.255986.5) (ISNI:0000 0004 0472 0419)
5 University of Michigan, Department of Physics, Ann Arbor, USA (GRID:grid.214458.e) (ISNI:0000000086837370)
6 Anhui University, Institute of Physical Science and Information Technology, Hefei, People’s Republic of China (GRID:grid.252245.6) (ISNI:0000 0001 0085 4987)
7 Chinese Academy of Sciences, Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Beijing, People’s Republic of China (GRID:grid.9227.e) (ISNI:0000000119573309)
8 Fudan University, State Key Laboratory of Surface Physics and Department of Physics, Shanghai, People’s Republic of China (GRID:grid.8547.e) (ISNI:0000 0001 0125 2443)
9 The University of Hong Kong, Department of Physics and HKU-UCAS Joint Institute for Theoretical and Computational Physics at Hong Kong, Hong Kong, China (GRID:grid.194645.b) (ISNI:0000000121742757); Fudan University, State Key Laboratory of Surface Physics and Department of Physics, Shanghai, People’s Republic of China (GRID:grid.8547.e) (ISNI:0000 0001 0125 2443)
10 University of Science and Technology of China, Hefei National Laboratory for Physical Sciences at Microscale, Department of Physics, and Key Laboratory of Strongly-Coupled Quantum Matter Physics (CAS), Hefei, People’s Republic of China (GRID:grid.59053.3a) (ISNI:0000000121679639); Anhui University, Institute of Physical Science and Information Technology, Hefei, People’s Republic of China (GRID:grid.252245.6) (ISNI:0000 0001 0085 4987)