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Measuring the Spin-Lattice Relaxation Magnetic Field Dependence of Hyperpolarized [1-13C]pyruvate
Published on: September 13, 2019
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Magnetic field-induced intermediate quantum spin liquid with a spinon Fermi surface
Niravkumar D Patel1, Nandini Trivedi2
1Department of Physics, The Ohio State University, Columbus, OH 43210.
Summary
The Kitaev model transitions from a gapped to a gapless quantum spin liquid (QSL) and then to a polarized phase under a magnetic field. Researchers identified the intermediate phase as a gapless U(1) QSL using DMRG.
Area of Science:
- Condensed Matter Physics
- Quantum Magnetism
- Topological Phases of Matter
Background:
- The Kitaev model describes a quantum spin liquid (QSL) state, a novel phase of matter with exotic properties.
- Understanding phase transitions in QSLs under external fields is crucial for exploring their potential applications.
Purpose of the Study:
- To investigate the phase transitions of the Kitaev model under an applied magnetic field.
- To identify the nature of the intermediate phase and characterize its properties.
Main Methods:
- Density matrix renormalization group (DMRG) method applied to large honeycomb clusters.
- Analysis of static spin-spin correlations, magnetization, spin susceptibility, specific heat, and entropy.
Main Results:
- Two magnetic field-induced transitions were observed in the Kitaev model.
- The intermediate phase was identified as a gapless U(1) quantum spin liquid (QSL).
- The spin structure function and Fermi surface of gapless spinons were determined.
Conclusions:
- The study elucidates the field-dependent phase diagram of the Kitaev model.
- The findings confirm the existence and characteristics of a gapless U(1) QSL phase.
- The results provide insights into the behavior of quantum spin liquids in magnetic fields.
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