Skyrmion defects and competing singlet orders in a half-filled antiferromagnetic Kondo-Heisenberg model on the honeycomb lattice
arXiv:1704.07818 · doi:10.1103/PhysRevB.96.125101
Abstract
Due to the interaction between topological defects of an order parameter and underlying fermions, the defects can possess induced fermion numbers, leading to several exotic phenomena of fundamental importance to both condensed matter and high energy physics. One of the intriguing outcome of induced fermion number is the presence of fluctuating competing orders inside the core of topological defect. In this regard, the interaction between fermions and skyrmion excitations of antiferromagnetic phase can have important consequence for understanding the global phase diagrams of many condensed matter systems where antiferromagnetism and several singlet orders compete. We critically investigate the relation between fluctuating competing orders and skyrmion excitations of the antiferromagnetic insulating phase of a half-filled Kondo-Heisenberg model on honeycomb lattice. By combining analytical and numerical methods we obtain exact eigenstates of underlying Dirac fermions in the presence of a single skyrmion configuration, which are used for computing induced chiral charge. Additionally, by employing this nonperturbative eigenbasis we calculate the susceptibilities of different translational symmetry breaking charge, bond and current density wave orders and translational symmetry preserving Kondo singlet formation. Based on the computed susceptibilities we establish spin Peierls and Kondo singlets as dominant competing orders of antiferromagnetism. We show favorable agreement between our findings and field theoretic predictions based on perturbative gradient expansion scheme which crucially relies on adiabatic principle and plane wave eigenstates for Dirac fermions. The methodology developed here can be applied to many other correlated systems supporting competition between spin-triplet and spin-singlet orders in both lower and higher spatial dimensions.
15 pages, 11 figures
References in corpus (16)
- Fermi-liquid instabilities at magnetic quantum phase transitions
- "Deconfined" quantum critical points
- Quantum criticality beyond the Landau-Ginzburg-Wilson paradigm
- Quantum criticality
- Heavy Fermions and Quantum Phase Transitions
- Weak magnetism and non-Fermi liquids near heavy-fermion critical points
- Evidence for deconfined quantum criticality in a two-dimensional Heisenberg model with four-spin interactions
- Electron fractionalization in two-dimensional graphenelike structures
- Algebraic spin liquid as the mother of many competing orders
- Many-body spin Berry phases emerging from the -flux state: antiferromagnetic/valence-bond-solid competition
- Fermi surface reconstruction and multiple quantum phase transitions in the antiferromagnet CeRhIn
- Characteristic signatures of quantum criticality driven by geometrical frustration
- Magnetic field tuned quantum criticality of heavy fermion system YbPtBi
- Geometric phases and competing orders in two dimensions
- Charge- Skyrmion condensate in a hidden order state
- Conserved charges of order-parameter textures in Dirac systems
Cited by in corpus (8)
- Ultrafast generation and dynamics of isolated skyrmions in antiferromagnetic insulators
- Antiferromagnetism emerging in a ferromagnet with gain
- Itinerant quantum multi-criticality of two dimensional Dirac fermions
- Quantum critical metals and loss of quasiparticles
- Statistical nature of Skyrme-Faddeev models in dimensions and normalizable fermions
- Color degeneracy of competing orders near topological defects cores in planar quadratic band touching systems
- Mechanism of skyrmion condensation and pairing for twisted bi-layer graphene
- Topological quantum control: Edge currents via Floquet depinning of skyrmions in the graphene quantum Hall antiferromagnet