2019
DOI: 10.1088/1361-648x/ab283e
|View full text |Cite
|
Sign up to set email alerts
|

Heisenberg–Kitaev physics in magnetic fields

Abstract: Magnetic insulators in the regime of strong spin-orbit coupling exhibit intriguing behaviors in external magnetic fields, reflecting the frustrated nature of their effective interactions.We review the recent advances in understanding the field responses of materials that are described by models with strongly bond-dependent spin exchange interactions, such as Kitaev's celebrated honeycomb model and its extensions. We discuss the field-induced phases and the complex magnetization processes found in these theorie… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1
1

Citation Types

6
104
0

Year Published

2020
2020
2024
2024

Publication Types

Select...
9

Relationship

0
9

Authors

Journals

citations
Cited by 133 publications
(114 citation statements)
references
References 155 publications
6
104
0
Order By: Relevance
“…By contrast, the phases from paths (ii) and (iii)-wherein the edge fermion encircles the bulk Ising anyon an even number of times-conform exactly to Eqs. (36) and (38), respectively [129]. In paths (iv) and (v), the incident emergent fermion splinters into two Ising anyons at the constriction, one of which now encircles a bulk Ising anyon.…”
Section: B Interferometer With a = σmentioning
confidence: 99%
“…By contrast, the phases from paths (ii) and (iii)-wherein the edge fermion encircles the bulk Ising anyon an even number of times-conform exactly to Eqs. (36) and (38), respectively [129]. In paths (iv) and (v), the incident emergent fermion splinters into two Ising anyons at the constriction, one of which now encircles a bulk Ising anyon.…”
Section: B Interferometer With a = σmentioning
confidence: 99%
“…but canted away from the [111] field. Such a canting originates from the competition between the field and the interaction [30,32,33], thus motivating the name frustrated ferromagnet (FF) for such a phase.…”
Section: Classical U(1) Degeneracy and Quantum Order-by-disordermentioning
confidence: 99%
“…In a field along the [111] axis, however, a tensor network study reveals that KSL is confined to the vicinity of the pure Kitaev model, while novel nematic paramagnetic states, which breaks the lattice-rotational symmetry, occupy a significant portion of the phase diagram at intermediate fields [31]. On the other hand, the classical model exhibits a plethora of magnetic orders with large unit cells, and a ferromagnetic phase frustrated by the interaction and the field, before the system becomes fully polarized [30,32,33].…”
Section: Introductionmentioning
confidence: 99%
“…Nonetheless, the gap between experiments and theoretical understanding is still apparent. Since the non-Kitaev interactions and magnetic field [31,32] spoil the exact solution and restrict QMC simulations to a relatively high temperature [33], little is known about the fractionalization of spins in the extended Kitaev models.…”
Section: Introductionmentioning
confidence: 99%