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Spectral Functions of an Extended Antiferromagnetic $S=1/2$ Heisenberg Model on the Triangular Lattice
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abstract
We study an extended spin-$1/2$ antiferromagnetic Heisenberg model on the triangular lattice, which includes both nearest- and next-nearest-neighbor interactions, as well as a scalar chiral term. This model exhibits a rich phase diagram featuring several competing phases: different quantum spin liquids and various magnetically ordered states, including coplanar $120^\circ$ order, stripe order, and non-coplanar tetrahedral order. We employ large-scale matrix product state simulations optimized for GPUs to obtain high-resolution dynamical responses. Our calculations reveal the spectral features across both ordered and liquid regimes of the phase diagram, which we analyze in comparison with analytical predictions and field-theoretical approaches. We identify unique signatures of the ordered phases in the form of gapless Goldstone modes at the ordering wave vectors. Our results in the $J_1-J_2$ quantum spin-liquid regime are indicative of a $U(1)$ Dirac spin liquid. In the chiral spin-liquid phase, we find signatures of spinons as the fractional excitations of the underlying theory, manifested as the onset of a two-spinon continuum that agrees with predictions from the Kalmeyer-Laughlin ansatz for the ground-state wave function, and collective modes that can be viewed as spinon bound states. We discuss finite-size effects, their consistency with the presumptions from field-theory, and review the dynamical structure factor with regard to experimentally relevant features such as the occurrence of highly dispersive signals and the global distribution of spectral weight.
Forward citations
Cited by 4 Pith papers
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Competing states in the $S=1/2$ triangular-lattice $J_1$-$J_2$ Heisenberg model: a dynamical density-matrix renormalization group study
In the triangular-lattice J1-J2 Heisenberg model at J2=0.12, the two low-energy states seen in DMRG are distinct competing phases—one Dirac-spin-liquid-like, one resembling 120-degree magnetic order—not a topological ...
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Valley-controlled chiral magnetism in transition metal dichalcogenide monolayers
In spin-valley-locked TMD monolayers, the RKKY interaction becomes a chiral coupling that selects a single chirality of the 120° Néel state and shifts the BKT transition to higher temperature.
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Dissipationless dynamics of spin supersolid states in a spin-1/2 triangular antiferromagnet with impurities
Impurities preserve the gapless Goldstone mode in spin supersolid phases but split magnon bands in the up-up-down phase, offering a spectroscopic probe of spin superfluidity.
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Emergent Spin Supersolids in Frustrated Quantum Materials
Spin supersolids featuring coexisting longitudinal spin order breaking lattice symmetry and transverse order breaking spin U(1) symmetry have been established in frustrated quantum magnets through consistent experimen...
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