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Title: BCS-BEC crossover in a (t2g)4 excitonic magnet

Abstract

The condensation of spin-orbit-induced excitons in t 2 g 4 electronic systems is attracting considerable attention. At large Hubbard U , antiferromagnetism was proposed to emerge from the Bose-Einstein Condensation (BEC) of triplons ( J eff = 1 ). Furthermore, we show that even at intermediate U regimes, the spin-orbit exciton condensation is possible leading also to staggered magnetic order. The canonical electron-hole excitations (excitons) transform into local triplon excitations at large U , and this BEC strong coupling regime is smoothly connected to the intermediate U excitonic insulator region. We solved the degenerate three-orbital Hubbard model with spin-orbit coupling ( λ ) in one dimension using the density matrix renormalization group, while in two dimensions we use the Hartree-Fock approximation (HFA). Employing these techniques, we provide the full λ versus U phase diagrams for both one- and two-dimensional lattices. Our main result is that at intermediate Hubbard U , increasing λ at fixed U the system transitions from an incommensurate spin-density-wave metal to a Bardeen-Cooper-Schrieffer (BCS) excitonic insulator, with coherence length r coh of O ( a ) and O ( 10 a ) in 1 d and 2 d , respectively, with a being the lattice spacing. Further increasing λ , the system eventually crosses over to the BEC limit (with r coh a ).

Authors:
 [1]; ORCiD logo [1];  [2]; ORCiD logo [3];  [1]
  1. University of Tennessee, Knoxville, TN (United States); Oak Ridge National Laboratory (ORNL), Oak Ridge, TN (United States)
  2. University of British Columbia, Vancouver, B.C. (Canada)
  3. Oak Ridge National Laboratory (ORNL), Oak Ridge, TN (United States)
Publication Date:
Research Org.:
Oak Ridge National Lab. (ORNL), Oak Ridge, TN (United States)
Sponsoring Org.:
USDOE Office of Science (SC), Basic Energy Sciences (BES). Materials Sciences & Engineering Division
OSTI Identifier:
1649072
Grant/Contract Number:  
AC05-00OR22725
Resource Type:
Accepted Manuscript
Journal Name:
Physical Review B
Additional Journal Information:
Journal Volume: 101; Journal Issue: 24; Journal ID: ISSN 2469-9950
Publisher:
American Physical Society (APS)
Country of Publication:
United States
Language:
English
Subject:
75 CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND SUPERFLUIDITY; BEC-BCS crossover; Excitons; Magnetism; Phase diagrams; Spin-orbit coupling; 1-dimensional systems; 2-dimensional systems; Density matrix renormalization group; Hubbard model

Citation Formats

Kaushal, Nitin, Soni, Rahul, Nocera, Alberto, Alvarez, Gonzalo, and Dagotto, Elbio R. BCS-BEC crossover in a (t2g)4 excitonic magnet. United States: N. p., 2020. Web. doi:10.1103/physrevb.101.245147.
Kaushal, Nitin, Soni, Rahul, Nocera, Alberto, Alvarez, Gonzalo, & Dagotto, Elbio R. BCS-BEC crossover in a (t2g)4 excitonic magnet. United States. https://doi.org/10.1103/physrevb.101.245147
Kaushal, Nitin, Soni, Rahul, Nocera, Alberto, Alvarez, Gonzalo, and Dagotto, Elbio R. Thu . "BCS-BEC crossover in a (t2g)4 excitonic magnet". United States. https://doi.org/10.1103/physrevb.101.245147. https://www.osti.gov/servlets/purl/1649072.
@article{osti_1649072,
title = {BCS-BEC crossover in a (t2g)4 excitonic magnet},
author = {Kaushal, Nitin and Soni, Rahul and Nocera, Alberto and Alvarez, Gonzalo and Dagotto, Elbio R.},
abstractNote = {The condensation of spin-orbit-induced excitons in t2g4 electronic systems is attracting considerable attention. At large Hubbard U, antiferromagnetism was proposed to emerge from the Bose-Einstein Condensation (BEC) of triplons (Jeff=1). Furthermore, we show that even at intermediate U regimes, the spin-orbit exciton condensation is possible leading also to staggered magnetic order. The canonical electron-hole excitations (excitons) transform into local triplon excitations at large U, and this BEC strong coupling regime is smoothly connected to the intermediate U excitonic insulator region. We solved the degenerate three-orbital Hubbard model with spin-orbit coupling (λ) in one dimension using the density matrix renormalization group, while in two dimensions we use the Hartree-Fock approximation (HFA). Employing these techniques, we provide the full λ versus U phase diagrams for both one- and two-dimensional lattices. Our main result is that at intermediate Hubbard U, increasing λ at fixed U the system transitions from an incommensurate spin-density-wave metal to a Bardeen-Cooper-Schrieffer (BCS) excitonic insulator, with coherence length rcoh of O(a) and O(10a) in 1d and 2d, respectively, with a being the lattice spacing. Further increasing λ, the system eventually crosses over to the BEC limit (with rcoh≪a).},
doi = {10.1103/physrevb.101.245147},
journal = {Physical Review B},
number = 24,
volume = 101,
place = {United States},
year = {Thu Jun 18 00:00:00 EDT 2020},
month = {Thu Jun 18 00:00:00 EDT 2020}
}

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