2016
DOI: 10.1103/physrevb.94.115112
|View full text |Cite
|
Sign up to set email alerts
|

Electronic quasiparticles in the quantum dimer model: Density matrix renormalization group results

Abstract: We study a recently proposed quantum dimer model for the pseudogap metal state of the cuprates.The model contains bosonic dimers, representing a spin-singlet valence bond between a pair of electrons, and fermionic dimers, representing a quasiparticle with spin-1/2 and charge +e. By density matrix renormalization group calculations on a long but finite cylinder, we obtain the ground-state density distribution of the fermionic dimers for a number of different total densities. From the Friedel oscillations at ope… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

3
12
0

Year Published

2016
2016
2019
2019

Publication Types

Select...
8

Relationship

2
6

Authors

Journals

citations
Cited by 12 publications
(15 citation statements)
references
References 22 publications
3
12
0
Order By: Relevance
“…Close to the V-M phase transition, equation (A.1) fails to describe the behavior of the EE, but sufficiently far away from the transition point the fit agrees well with the numerical data. Such EE behavior has also been observed in other models [34,55,[78][79][80], and is ascribed to the fact that in the vicinity of the phase transition, the low-energy excitations become massive because of the presence of a gapped low-energy spectrum, and the leading order of S ℓ ( ) is not described by equation (A.1) any more. We show the central charge as a function of U J 2 ( ), for the same set of data, in panels (c) and (d).…”
Section: Appendix a Numerical Analysis Of The Phase Diagramsupporting
confidence: 70%
“…Close to the V-M phase transition, equation (A.1) fails to describe the behavior of the EE, but sufficiently far away from the transition point the fit agrees well with the numerical data. Such EE behavior has also been observed in other models [34,55,[78][79][80], and is ascribed to the fact that in the vicinity of the phase transition, the low-energy excitations become massive because of the presence of a gapped low-energy spectrum, and the leading order of S ℓ ( ) is not described by equation (A.1) any more. We show the central charge as a function of U J 2 ( ), for the same set of data, in panels (c) and (d).…”
Section: Appendix a Numerical Analysis Of The Phase Diagramsupporting
confidence: 70%
“…However, if the confinement length scale is very large, the fermions should effectively realize a U (1) FL* state. This picture of an effective deconfined phase has been supported by DMRG studies of a particular dimer model of the U (1) FL* [31].…”
Section: Model Of Z 2 -Fl* With Bosonic Chargonsmentioning
confidence: 65%
“…Most of the numerical results in the present paper have been obtained with a Density Matrix Renormalization Group (DMRG) algorithm [15][16][17], while most of the earlier numerical investigations of quantum dimer models in the context of 2D models have been performed either with exact diagonalizations (ED) or Quantum Monte Carlo (QMC). When DMRG has been used, the quantum dimer constraint has not been encoded explicitly, but through an additional term in the Hamiltonian that penalizes energetically the states that do not satisfy the local constraints of the model [11,18,19]. In this section we explain how to explicitly implement the local constraint in a variational Matrix Product States (MPS) algorithm.…”
Section: Fibonacci Anyon Chainmentioning
confidence: 99%