Long-range magnetic order in models for rare-earth quasicrystals
Physical Review B American Physical Society (APS) 92:22 (2015) 224409
Neutron scattering signatures of the 3D hyperhoneycomb Kitaev quantum spin liquid
Physical review B: Condensed matter and materials physics American Physical Society 92:18 (2015) ARTN 180408
Abstract:
Motivated by recent synthesis of the hyperhoneycomb material β−Li2IrO3, we study the dynamical structure factor (DSF) of the corresponding 3D Kitaev quantum spin-liquid (QSL), whose fractionalized degrees of freedom are Majorana fermions and emergent flux loops. The properties of this 3D model are known to differ in important ways from those of its 2D counterpart—it has a finite-temperature phase transition, as well as distinct features in the Raman response. We show, however, that the qualitative behavior of the DSF is broadly dimension-independent. Characteristics of the 3D DSF include a response gap even in the gapless QSL phase and an energy dependence deriving from the Majorana fermion density of states. Since the majority of the response is from states containing a single Majorana excitation, our results suggest inelastic neutron scattering as the spectroscopy of choice to illuminate the physics of Majorana fermions in Kitaev QSLs.Deconfined Quantum Criticality, Scaling Violations, and Classical Loop Models
Physical Review X American Physical Society (APS) 5:4 (2015) 041048
Dynamics of fractionalization in quantum spin liquids
Physical review B: Condensed matter and materials physics American Physical Society 92:11 (2015) ARTN 115127
Abstract:
We present the theory of dynamical spin response for the Kitaev honeycomb model, obtaining exact results for the structure factor (SF) in gapped and gapless, Abelian and non-Abelian quantum spin-liquid (QSL) phases. We also describe the advances in methodology necessary to compute these results. The structure factor shows signatures of spin fractionalization into emergent quasiparticles: Majorana fermions and fluxes of Z2 gauge field. In addition to a broad continuum from spin fractionalization, we find sharp (δ-function) features in the response. These arise in two distinct ways: from excited states containing only (static) fluxes and no (mobile) fermions, and from excited states in which fermions are bound to fluxes. The SF is markedly different in Abelian and non-Abelian QSLs, and bound fermion-flux composites appear only in the non-Abelian phase.Passive correction of quantum logical errors in a driven, dissipative system: A blueprint for an analog quantum code fabric
Physical Review A American Physical Society (APS) 91:6 (2015) 062324