Topological quantum phase transition in strongly correlated Kondo insulators in 1D

We investigate, by means of a eld-theory analysis combined with the density-matrix renormalization group (DMRG) method, a theoretical model for a strongly correlated quantum system in one dimension realizing a topologically-ordered Haldane phase ground state.The model consists of a spin-1/2 Heisenbe...

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Bibliographic Details
Authors: Lisandrini, Franco Thomas, Lobos, Alejandro Martin, Dobry, Ariel Oscar, Gazza, Claudio Javier
Format: article
Status:Published version
Publication Date:2016
Country:Argentina
Institution:Consejo Nacional de Investigaciones Científicas y Técnicas
Repository:CONICET Digital (CONICET)
Language:English
OAI Identifier:oai:ri.conicet.gov.ar:11336/50534
Online Access:http://hdl.handle.net/11336/50534
Access Level:Open access
Keyword:topological insulators
Kondo Insulators
correlated electron systems
DMRG
https://purl.org/becyt/ford/1.3
https://purl.org/becyt/ford/1
Description
Summary:We investigate, by means of a eld-theory analysis combined with the density-matrix renormalization group (DMRG) method, a theoretical model for a strongly correlated quantum system in one dimension realizing a topologically-ordered Haldane phase ground state.The model consists of a spin-1/2 Heisenberg chain coupled to a tight-binding chain via two competing Kondo exchange couplings of dierent type: a "s-wave" Kondo coupling (JsK), and a less common "p-wave" (JpK) Kondo coupling. While the first coupling is the standard Kondo interaction studied in many condensed-matter systems, the latter has been recently introduced by Alexandrov and Coleman [Phys. Rev. B 90, 115147 (2014)] as a possible mechanism leading to a topological Kondo-insulating ground state in one dimension. As a result of this competition, a topological quantum phase transition (TQPT) occurs in the system for a critical value of the ratio JsK/JpK, separating a (Haldane-type) topological phase from a topologically trivial ground state where the system can be essentially described as a product of local singlets. We study and characterize the TQPT by means of the magnetization prole, the entanglement entropy and the full entanglement spectrum of the ground state. Our results might be relevant to understand howtopologically-ordered phases of fermions emerge in strongly interacting quantum systems.