Spectra of a gapped quantum spin liquid with a strong chiral excitation on the triangular lattice
Source abstract
Abstract
Whereas a quantum spin liquid (QSL) phase has been identified in the ${J}1\text{\ensuremath{-}}{J}2$ Heisenberg model on a triangular lattice via numerical calculations, debate persists about whether or not such a QSL is gapped or gapless with contradictory conclusions from different techniques. Moreover, information about excitations and dynamics is crucial for the experimental detection of such a phase. In this paper, we use exact diagonalization to characterize signatures of a QSL phase on the triangular lattice through the dynamical spin structure factor $\mathcal{S}(q,\ensuremath{\omega})$ and Raman susceptibility $\ensuremath{\chi}(\ensuremath{\omega})$. We find that spectra for the QSL phase show distinct features compared to those of neighboring phases; and both the Raman spectra and spin structure factor show gapped behavior in the QSL phase. Interestingly, there is a prominent excitation mode in the Raman ${A}2$ channel, indicating a strong subleading tendency toward a chiral spin liquid phase.
Source: openalex_inverted_index · Quality: baseline
Research context
OpenAlex topics: Advanced Condensed Matter Physics · Physics of Superconductivity and Magnetism · Quantum many-body systems
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
Affiliations
Department of Applied Physics, Stanford University, California 94305, USA
Stanford Institute for Materials and Energy Sciences, SLAC National Accelerator Laboratory, 2575 Sand Hill Road, Menlo Park, California 94025, USA
Department of Materials Science and Engineering, Stanford University, Stanford, California 94305, USA
Geballe Laboratory for Advanced Materials, Stanford University, Stanford, California 94305, USA
Funding
U.S. Department of Energy
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