Search arXiv⌕ Search

arXiv · 0911.5623

Exact results for the star lattice chiral spin liquid

Abstract

We examine the star lattice Kitaev model whose ground state is a a chiral spin liquid. We fermionize the model such that the fermionic vacua are toric code states on an effective Kagome lattice. This implies that the Abelian phase of the system is inherited from the fermionic vacua and that time reversal symmetry is spontaneously broken at the level of the vacuum. In terms of these fermions we derive the Bloch-matrix Hamiltonians for the vortex free sector and its time reversed counterpart and illuminate the relationships between the sectors. The phase diagram for the model is shown to be a sphere in the space of coupling parameters around the triangles of the lattices. The abelian phase lies inside the sphere and the critical boundary between topologically distinct Abelian and non-Abelian phases lies on the surface. Outside the sphere the system is generically gapped except in the planes where the coupling parameters are zero. These cases correspond to bipartite lattice structures and the dispersion relations are similar to that of the original Kitaev honeycomb model. In a further analysis we demonstrate the three-fold non-Abelian groundstate degeneracy on a torus by explicit calculation.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

G. Kells, D. Mehta, J. K. Slingerland, J. Vala. 2010-04-07. Exact results for the star lattice chiral spin liquid. https://doi.org/10.1103/physrevb.81.104429

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related papers

Quantum Theory of Exciton Magnetic Moment: Interaction and Topological Effects

Combining magnetometry with optical spectroscopy has uncovered novel quantum phenomena and is emerging as a powerful probe of quantum materials. However, the theory of the magnetic response of excitons, correlated electron-hole pairs in insulators, remains incomplete due to insufficient treatment of electron-hole interactions and quantum geometric effects. In biased bilayer graphene, for instance, theoretical predictions of valley g-factors for p-excitons deviate from experiment by nearly an order of magnitude. Here, we develop a quantum theory of the exciton orbital magnetic moment, based on first-order perturbation theory within the GW plus Bethe-Salpeter Equation approach and a rigorous treatment of the position operator in the response of exciton states to a magnetic field. Our formalism reveals three distinct contributions that go beyond the heuristic approaches used in the literature: a Berry-phase-corrected single-particle electron and hole moment difference, a term from envelope-function winding linked to electron-hole relative motion, and a center-of-mass correction from exciton band quantum geometry, with the latter two being completely new effects not considered in previous studies. Our ab initio calculations yield results in excellent agreement with experiment, establishing the importance of interaction and quantum geometric effects in the magnetic response of excitons.

cond-mat.mes-hall↗

Floquet-Multiple Andreev Reflections

Floquet theory describes quantum systems governed by time-periodic Hamiltonians, much as Bloch theory describes spatially periodic solids. In voltage-biased multiterminal Josephson junctions, the Josephson relation causes superconducting phase differences to evolve periodically in time, thereby providing an intrinsic Floquet drive. In this Letter, we consider three-terminal Josephson junctions formed on a ballistic two-dimensional normal conductor with a continuum of electronic states. We show that the quartet and higher-order multipair processes yield characteristic Floquet-multiple Andreev reflection (Floquet-MAR) finite-bias conductance and noise resonances that are parameterized by the bias voltage and electrochemical potential. This microscopic picture opens a route toward implementing and probing Floquet-MAR physics in ballistic multiterminal Josephson junctions.

cond-mat.mes-hall↗

Anomalous Transverse Thomson Effect

We formulate the anomalous transverse Thomson effect (ATTE), the long-missing Thomson counterpart of the anomalous Hall and anomalous Nernst effects. Its coefficient is not unique but depends on the electrical boundary condition: $τ_{\rm ATTE}^{(j)}$, defined for a spatially uniform imposed current density, and $τ_{\rm ATTE}^{(E)}$, defined for equipotential electrodes. Both are fully determined by the total anomalous Nernst coefficient (ANC) and its temperature dependence, while $τ_{\rm ATTE}^{(E)}$ acquires an additional contribution from the temperature dependence of the longitudinal resistivity. This relation is model independent within local linear response and applies to the total ANC regardless of whether its microscopic origin is intrinsic or extrinsic. Using a massive Dirac model for Fe$_3$Sn$_2$, we show that Berry curvature near the gapped Dirac cones enhances the ANC-related contributions to $τ_{\rm ATTE}^{(E)}$. In the low-temperature limit, both $τ_{\rm ATTE}^{(j)}/S_{xy}^{\rm A}$ and $τ_{\rm ATTE}^{(E)}/S_{xy}^{\rm A}$ approach a value of three. We further extract $τ_{\rm ATTE}^{(E)}$ from reported experimental data for CoS\(_2\), Co\(_3\)Sn\(_2\)S\(_2\) and CeCrGe\(_3\); for CeCrGe$_3$ it reaches approximately -20 $μV/K$, and we estimate the maximum achievable cold-side heat current density to assess its cooling potential. Because the ATTE can be evaluated directly from existing ANC and longitudinal resistivity data, it is readily testable without additional equipment or measurements.

cond-mat.mes-hall↗