2015
DOI: 10.1103/physrevb.91.125128
|View full text |Cite
|
Sign up to set email alerts
|

Theoretical prediction of fragile Mott insulators on plaquette Hubbard lattices

Abstract: Employing extensive cellular dynamical mean-field theory (CDMFT) calculations with exact diagonalization impurity solver, we investigate the ground state phase diagrams and non-magnetic metal-insulator transitions of the half-filled Hubbard model on two plaquette -the 1/5 depleted and checkerboard -square lattices. We identify three different insulators in the phase diagrams: dimer insulator, antiferromagnetic insulator, and plaquette insulator. And we demonstrate that the plaquette insulator is a novel fragil… 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

0
6
0

Year Published

2016
2016
2022
2022

Publication Types

Select...
5
1

Relationship

2
4

Authors

Journals

citations
Cited by 7 publications
(6 citation statements)
references
References 43 publications
0
6
0
Order By: Relevance
“…First-principles calculations indicate that such a planar structure is kinetically stable at low temperature [12,13] and that its energy is a local minimum [12], which suggests that the material can potentially be synthesized in laboratories. Actually, this lattice structure has attracted a lot of research interest recently because it not only is hosted by quite a few real materials [14][15][16][17] but also has various intriguing phases on this lattice that have been revealed by theoretical calculations [18][19][20][21][22][23][24][25][26][27][28][29][30][31][32][33][34][35]. Here we notice another remarkable property of this 2D lattice: its band structure can have perfect Fermisurface (FS) nesting in a wide parameter regime at half filling, which easily leads to antiferromagnetic SDW order.…”
Section: Introductionmentioning
confidence: 99%
“…First-principles calculations indicate that such a planar structure is kinetically stable at low temperature [12,13] and that its energy is a local minimum [12], which suggests that the material can potentially be synthesized in laboratories. Actually, this lattice structure has attracted a lot of research interest recently because it not only is hosted by quite a few real materials [14][15][16][17] but also has various intriguing phases on this lattice that have been revealed by theoretical calculations [18][19][20][21][22][23][24][25][26][27][28][29][30][31][32][33][34][35]. Here we notice another remarkable property of this 2D lattice: its band structure can have perfect Fermisurface (FS) nesting in a wide parameter regime at half filling, which easily leads to antiferromagnetic SDW order.…”
Section: Introductionmentioning
confidence: 99%
“…33,44 The models should be also gapped at half-filling. Thus, the checkerboard Hubbard model 50 and the Hubbard model on the 1/5-depleted square lattice 51 in two dimensions are good candidates. We also note that the Hubbard U is tunable for ultracold fermionic atoms in an optical lattice, [52][53][54][55] which provides a good experimental setting to observe the Nagaoka polaron and MBL studied here.…”
Section: Discussionmentioning
confidence: 99%
“…The standard multi-orbital RPA [74][75][76][77][78][79][80][81][82][83][84][85][86] approach was used to treat the weak-coupling limit of the model. The largest pairing eigenvalue λ is used to estimate T c by the following equation: [79,87] λ…”
Section: Weak-coupling Limitmentioning
confidence: 99%
“…[15] [15] 4.3. Strong-coupling limit In the strong-coupling limit, the Hubbard model becomes an effective t-J model [86] H…”
Section: Intermediate-couplingmentioning
confidence: 99%