Quantum exotic states in correlated topological insulators Su-Peng Kou ( 寇谡鹏 ) Beijing Normal University.

Slides:



Advertisements
Similar presentations
Anyon and Topological Quantum Computation Beijing Normal university
Advertisements

High T c Superconductors & QED 3 theory of the cuprates Tami Pereg-Barnea
Phase structure of topological insulators by lattice strong-coupling expansion Yasufumi Araki (The Univ. of Texas at Austin) Jul Aug. 3, 2013: Lattice.
Quantum “disordering” magnetic order in insulators, metals, and superconductors HARVARD Talk online: sachdev.physics.harvard.edu Perimeter Institute, Waterloo,
Kun Yang National High Magnetic Field Lab and Florida State University
D-wave superconductivity induced by short-range antiferromagnetic correlations in the Kondo lattice systems Guang-Ming Zhang Dept. of Physics, Tsinghua.
Zheng-Yu Weng Institute for Advanced Study Tsinghua University, Beijing Newton Institute, Cambridge Mott Physics, Sign Structure, and High-Tc.
Coherence, Dynamics, Transport and Phase Transition of Cold Atoms Wu-Ming Liu (刘伍明) (Institute of Physics, Chinese Academy of Sciences)
Quantum critical phenomena Talk online: sachdev.physics.harvard.edu Talk online: sachdev.physics.harvard.edu Quantum critical phenomena Talk online: sachdev.physics.harvard.edu.
Quantum anomalous Hall effect (QAHE) and the quantum spin Hall effect (QSHE) Shoucheng Zhang, Stanford University Les Houches, June 2006.
Subir Sachdev Science 286, 2479 (1999). Quantum phase transitions in atomic gases and condensed matter Transparencies online at
Subir Sachdev arXiv: Subir Sachdev arXiv: Loss of Neel order in insulators and superconductors Ribhu Kaul Max Metlitski Cenke Xu.
Twist liquids and gauging anyonic symmetries
Fermi-Liquid description of spin-charge separation & application to cuprates T.K. Ng (HKUST) Also: Ching Kit Chan & Wai Tak Tse (HKUST)
Fractional topological insulators
Fractional Quantum Hall states in optical lattices Anders Sorensen Ehud Altman Mikhail Lukin Eugene Demler Physics Department, Harvard University.
Anomalous excitation spectra of frustrated quantum antiferromagnets John Fjaerestad University of Queensland Work done in collaboration with: Weihong Zheng,
Quick and Dirty Introduction to Mott Insulators
Fermionic Symmetry Protected Topological Phase Induced by Interaction Shangqiang NING First year PHD student Institute For Advanced Study, Tsinghua University.
THE STATE UNIVERSITY OF NEW JERSEY RUTGERS Studies of Antiferromagnetic Spin Fluctuations in Heavy Fermion Systems. G. Kotliar Rutgers University. Collaborators:
Classifying two-dimensional superfluids: why there is more to cuprate superconductivity than the condensation of charge -2e Cooper pairs cond-mat/ ,
Putting competing orders in their place near the Mott transition cond-mat/ and cond-mat/ Leon Balents (UCSB) Lorenz Bartosch (Yale) Anton.
Magnetic quantum criticality Transparencies online at Subir Sachdev.
Topological Insulators and Beyond
Localization of phonons in chains of trapped ions Alejandro Bermúdez, Miguel Ángel Martín-Delgado and Diego Porras Department of Theoretical Physics Universidad.
@Nagoya U. Sept. 5, 2009 Naoto Nagaosa Department of Applied Physics
Composite Fermion Groundstate of Rashba Spin-Orbit Bosons Alex Kamenev Fine Theoretical Physics Institute, School of Physics & Astronomy, University of.
Dung-Hai Lee U.C. Berkeley Quantum state that never condenses Condense = develop some kind of order.
Non-Fermi liquid vs (topological) Mott insulator in electronic systems with quadratic band touching in three dimensions Igor Herbut (Simon Fraser University,
Hadron to Quark Phase Transition in the Global Color Symmetry Model of QCD Yu-xin Liu Department of Physics, Peking University Collaborators: Guo H., Gao.
Effects of Interaction and Disorder in Quantum Hall region of Dirac Fermions in 2D Graphene Donna Sheng (CSUN) In collaboration with: Hao Wang (CSUN),
Photonic Topological Insulators
Zheng-Yu Weng IAS, Tsinghua University
1 Quantum Choreography: Exotica inside Crystals Electrons inside crystals: Quantum Mechanics at room temperature Quantum Theory of Solids: Band Theory.
The Helical Luttinger Liquid and the Edge of Quantum Spin Hall Systems
(Simon Fraser University, Vancouver)
Mott phases, phase transitions, and the role of zero-energy states in graphene Igor Herbut (Simon Fraser University) Collaborators: Bitan Roy (SFU) Vladimir.
Topology induced emergent dynamic gauge theory in an extended Kane-Mele-Hubbard model Xi Luo January 5, 2015 arXiv:
Non-Abelian Josephson effect and fractionalized vortices Wu-Ming Liu (刘伍明) ( Institute of Physics, CAS )
Topological insulators: interaction effects and new states of matter Joseph Maciejko PCTS/University of Alberta CAP Congress, Sudbury June 16, 2014.
Three Discoveries in Underdoped Cuprates “Thermal metal” in non-SC YBCO Sutherland et al., cond-mat/ Giant Nernst effect Z. A. Xu et al., Nature.
Oct. 26, 2005KIAS1 Competing insulating phases in one-dimensional extended Hubbard models Akira Furusaki (RIKEN) Collaborator: M. Tsuchiizu (Nagoya) M.T.
Exact ground states of a frustrated 2D magnet: deconfined fractional excitations at a first order quantum phase transition Cristian D. Batista and Stuart.
Hidden topological order in one-dimensional Bose Insulators Ehud Altman Department of Condensed Matter Physics The Weizmann Institute of Science With:
Deconfined quantum criticality Leon Balents (UCSB) Lorenz Bartosch (Frankfurt) Anton Burkov (Harvard) Matthew Fisher (UCSB) Subir Sachdev (Harvard) Krishnendu.
The Puzzling Boundaries of Topological Quantum Matter Michael Levin Collaborators: Chien-Hung Lin (University of Chicago) Chenjie Wang (University of Chicago)
Deconfined quantum criticality T. Senthil (MIT) P. Ghaemi,P. Nikolic, M. Levin (MIT) M. Hermele (UCSB) O. Motrunich (KITP), A. Vishwanath (MIT) L. Balents,
The Landscape of the Hubbard model HARVARD Talk online: sachdev.physics.harvard.edu Subir Sachdev Highly Frustrated Magnetism 2010 Johns Hopkins University.
Functional Integration in many-body systems: application to ultracold gases Klaus Ziegler, Institut für Physik, Universität Augsburg in collaboration with.
Lattice gauge theory treatment of Dirac semimetals at strong coupling Yasufumi Araki 1,2 1 Institute for Materials Research, Tohoku Univ. 2 Frontier Research.
Flat Band Nanostructures Vito Scarola
1 Vortex configuration of bosons in an optical lattice Boulder Summer School, July, 2004 Congjun Wu Kavli Institute for Theoretical Physics, UCSB Ref:
Quantum spin Hall effect Shoucheng Zhang (Stanford University) Collaborators: Andrei Bernevig, Congjun Wu (Stanford) Xiaoliang Qi (Tsinghua), Yongshi Wu.
DISORDER AND INTERACTION: GROUND STATE PROPERTIES of the DISORDERED HUBBARD MODEL In collaboration with : Prof. Michele Fabrizio and Dr. Federico Becca.
From fractionalized topological insulators to fractionalized Majoranas
Fractional Berry phase effect and composite particle hole liquid in partial filled LL Yizhi You KITS, 2017.
Spin-Orbit Coupling Effects in Bilayer and Optical Lattice Systems
Boris Altshuler Physics Department, Columbia University Collaboration:
Quantum vortices and competing orders
Topological Insulators
Quantum Hall Fluids By Andrew York 12/5/2008.
Experimental Evidences on Spin-Charge Separation
Quantum phases and critical points of correlated metals
10 Publications from the project
Topological Order and its Quantum Phase Transition
Deconfined quantum criticality
Chengfu Mu, Peking University
SOC Fermi Gas in 1D Optical Lattice —Exotic pairing states and Topological properties 中科院物理研究所 胡海平 Collaborators : Chen Cheng, Yucheng Wang, Hong-Gang.
Hyun Kyu Lee Hanyang University
Exotic magnetic states in two-dimensional organic superconductors
Presentation transcript:

Quantum exotic states in correlated topological insulators Su-Peng Kou ( 寇谡鹏 ) Beijing Normal University

Outline Motivation Motivation Topological spin density waves in correlated topological insulators Topological spin density waves in correlated topological insulators Quantum spin liquid states in correlated topological insulators Quantum spin liquid states in correlated topological insulators Conclusion Conclusion [1] Kou SP , PHYS. REV. B 78, ( 2008 ). [2] Sun GY and Kou SP, EPL, (2009). [3] Kou SP, and Liu LF , EUR. PHYS. J. B. 81, 165 (2011). [4] Sun GY and Kou SP, J. Phys. C 23 (2011) [5] He J, Kou SP, Liang Y, Feng SP, PHYS. REV. B 83, (2011). [6] He J, Zong YH, Kou SP, Liang Y, Feng SP, PHYS. REV. B 84, (2011). [7] He J, Liang Y, Kou SP, PHYS. REV. B. 85, (2012). [8] He J, Wang B, Kou SP, PHYS. REV. B. submitted, arXiv: [9] Kou SP, “ Insulators: Types, Properties and Uses ” (Nova Science Publishers).

Look for quantum exotic states in correlated topological insulator I. Motivation: Look for quantum exotic states in correlated topological insulator X. G. Wen, Quantum Field Theory of Many-Body Systems

Spin liquid – emergent in physics No broken symmetry Deconfined spinons + Spin liquid Emergent gauge field +

Spin orders in strongly correlated electron systems G. Misguich, arXiv:cond-mat/

II. Topological spin density wave states in correlated topological insulators Instability of an interacting fermion system with topologically nontrivial band structure 1.Interacting spinful Haldane model 2.Interacting Kane-Mele model

The spinful Haldane model – spin rotation symmetry, no T symmetry

The Kane-Mele model – T symmetry, no spin rotation symmetry Kane and Mele, Phys. Rev. Lett. 95, (2005)

Possible quantum spin liquid in the interacting Kane-Mele model – T symmetry, no spin rotation symmetry Slave-rotor theory: Stephan Rachel and Karyn Le Hury, Phys. Rev. B (2010) QMC: M. Hohenadler, T. C. Lang, F. F. Assaad, Phys. Rev. Lett. 106, (2011) Dong Zheng, Congjun Wu and Guang-Ming Zhang, Phys. Rev. B 84, (2011) VCA : Shun-Li Yu, X.C. Xie, Jian-Xin Li, Phys. Rev. Lett. 107, (2011) DMF: Wei Wu, S. Rachel, Wu-Ming Liu, K. Le Hur, Phys. Rev. B 85, (2012)

Topological spin-density-wave states in interacting spinful Haldane model 1. Topological spin-density-wave states in interacting spinful Haldane model - spin rotation symmetry, no T symmetry He J, Zong YH, Kou SP, Liang Y, Feng SP, PHYS. REV. B 84, (2011) What is the ground state for the spinful Haldane model with the on-site interaction?

Mean field equation where Mean field approach M is the staggered magnetization.

Phase diagram C=2 topological insulator - QAH Band insulator Trivial AF-SDW order B-type topological SDW order A-type topological SDW order

Low energy effective model

K-matrix formulation

Spin-charge separated charge- flux binding effect in A-TSDW

spin-charge synchronization charge- flux binding effect in B-TSDW

Different spin-density-wave states in correlated topological insulators with the same local order parameter may have different topological properties, including the induced quantum numbers on topological objects, the edge states, the quantum Hall effects.

2. Quantum spin orders in correlated topological insulator with flat-band

Possible fractional quanum hall states

1.What is the ground state for the correlated topological insulators in the flat- band limit? 2.What’s the dispersion of electrons and spin waves for correlated topological insulators in the flat-band limit?

Phase diagram : electrons on TFB d is the hole concentration. FM (topological) spin-density-wave

Dispersion of electrons in A-TSDW Dispersion of spin-waves in A-TSDW A-TSDW : Half filling case A-TSDW AF-SDW TFB

FM (topological) spin-density-wave: quarter filling case Dispersion of electrons in FM order Dispersion of spin wave in FM order

FM order and AF order : d=0.3 filling case Dispersion of electrons Order parameters

III. Quantum spin liquids in interacting spinful Haldane model Short range A-type topological spin density wave state: chiral spin liquid Short range A-type topological spin density wave state: chiral spin liquid Short range B-type topological spin density wave state : composite spin liquid Short range B-type topological spin density wave state : composite spin liquid

Quantum spin-fluctuations in topological spin density wave states Transverse spin susceptibility is Spin coupling constant Spin wave velocity X. G. Wen, Quantum Field Theory of Many-Body Systems, (Oxford Univ. Press, Oxford, 2004) One obtains spin stiffness and the transverse spin susceptibility: H.J. Schulz, in The hubbard Model, edited by D. Baeriswyl(Plenum, New York, 1995). Z. Y. Weng, C. S. Ting, and T. K. Lee, Phys. Rev. B43, 3790 (1991). K. Borejsza, N. Dupuis, Euro Phys. Lett. 63, 722 (2003); Phys. Rev. B 69, (2004).

Spin coupling constant t’=0.0228t t’=0.1t

? ? ?

What is the nature of the quantum disordered states for TSDWs? S. Chakravarty, et al., Phys. Rev. B 39, 2344 (1989).

He J, Liang Y, Kou SP, PHYS. REV. B. 85, (2012).

Properties of chiral spin liquid Spinon is semion with fractional statistics Spinon is semion with fractional statistics Ground state degeneracy : 2 on torus Ground state degeneracy : 2 on torus Chiral gapless edge states Chiral gapless edge states He J, Liang Y, Kou SP, PHYS. REV. B. 85, (2012). X. G.Wen, F.Wilczek, and A. Zee, Phys. Rev. B 39, (1989).

Slave-rotor approach

Mean field approach

C=2 topological insulator Chiral spin liquid Trvial AF order A-TSDW

Chiral spin order parameter

π- vortex is semion Statistics angle θ = π/2 With induced fermion number, π-vortex becomes semion. With induced fermion number, π-vortex becomes semion.

Effective Lagrangian from slave-rotor approach N = 4

? S=1/2, charge e fermion

Composite spin liquidspin liquid

g > g c g < g c S=1/2, charge e fermion ?

To be confirmed by QMC, … IV. Conclusion ?

Thanks for your attention!

Spin susceptility of spin order in metallic spin order

1. Spin liquid 1. Spin liquid in the π-flux Hubbard model and the Hubbard model on honeycomb lattice

Quantum spin liquid near Mott transition of π- flux Hubbard model Sun GY and Kou SP, EPL, (2009). Kou SP, Liu LF, He J, Wu YJ , EUR. PHYS. J. B. 81, 165 (2011).

Gapless Z2 topological spin liquid There are three types of quasi-particles : gapped fermionic spinons, gapped bosonic spinons and the gapped gauge field.

Nodal spin liquid There are three types of quasi-particles : gapless fermionic spinons, gapped bosonic spinons and the roton- like gauge field.

Results from QMC Chia-Chen Chang and Richard T. Scalettar, Phys. Rev. Lett. 109, (2012)

Global Phase diagram by spin-fluctuation theory Sun GY and Kou SP, J. Phys. C. 23 (2011)

Quantum spin liquid from QMC Z. Y. Meng, T. C. Lang, S. Wessel, F. F. Assaad & A. Muramatsu, Nature 464, 847 (2010)

Results of the Hubbard Model on the Honeycomb Lattice from QMC of bigger size Sandro SorellaSandro Sorella, Yuichi Otsuka, Seiji Yunoki, arXiv: Yuichi OtsukaSeiji Yunoki