2021
DOI: 10.1103/physrevb.104.144406
|View full text |Cite
|
Sign up to set email alerts
|

Gutzwiller projected states for the J1J2 Heisenberg model on the Kagome lattice: Achievements and pitfalls

Abstract: We assess the ground-state phase diagram of the J1-J2 Heisenberg model on the kagome lattice by employing Gutzwiller-projected fermionic wave functions. Within this framework, different states can be represented, defined by distinct unprojected fermionic Hamiltonians that include hopping and pairing terms, as well as a coupling to local Zeeman fields to generate magnetic order. For J2 = 0, the so-called U(1) Dirac state, in which only hopping is present (such as to generate a π-flux in the hexagons), has been … Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

1
5
0

Year Published

2021
2021
2023
2023

Publication Types

Select...
6
2

Relationship

1
7

Authors

Journals

citations
Cited by 19 publications
(7 citation statements)
references
References 50 publications
1
5
0
Order By: Relevance
“…Thus, the system is expected to exhibit the Q = 0, 120 • order for J 2 > 0 and the √ 3 × √ 3 120 • order for J 2 < 0. This finding is consistent with previous studies [37][38][39]. Schematic views of these magnetic structures are presented in Fig.…”
Section: A Specific Heat and Entropysupporting
confidence: 93%
See 1 more Smart Citation
“…Thus, the system is expected to exhibit the Q = 0, 120 • order for J 2 > 0 and the √ 3 × √ 3 120 • order for J 2 < 0. This finding is consistent with previous studies [37][38][39]. Schematic views of these magnetic structures are presented in Fig.…”
Section: A Specific Heat and Entropysupporting
confidence: 93%
“…In the model compounds, the next-nearest-neighbor exchange interaction J 2 always exists regardless of whether it is large or small. The ground state of the J 1 − J 2 kagome lattice has been studied theoretically [37][38][39]. For J 2 > 0, the ground state exhibits a Q = 0, 120 • structure, whereas for J 2 < 0, the ground state exhibits a √ 3 × √ 3 120 • structure.…”
Section: Introductionmentioning
confidence: 99%
“…The vector M i effectively acts as a staggered magnetic field and magnetic order can be induced on top of the CSL state if h = 0 variationally [55,56]. In this situation, the spinon spectrum is gapped and we interpret the resulting state as adiabatically connected to a conventional magnetically ordered one.…”
Section: Variational Monte Carlo Resultsmentioning
confidence: 96%
“…The vector M i effectively acts as a staggered magnetic field and magnetic order can be induced on top of the CSL state if h = 0 variationally [46,47]. In this situation, the spinon spectrum is gapped and we interpret the resulting state as adiabatically connected to a conventional magnetically ordered one.…”
Section: Parton Mean-field Theory For Gapless Chiral Spin Liquidmentioning
confidence: 96%