Location via proxy:   [ UP ]  
[Report a bug]   [Manage cookies]                

Fractionalized quantum spin Hall effect

Michael W. Young, Sung-Sik Lee, and Catherine Kallin
Phys. Rev. B 78, 125316 – Published 15 September 2008

Abstract

Effects of electron correlations on a two-dimensional quantum spin Hall (QSH) system are studied. We examine possible phases of a generalized Hubbard model on a bilayer honeycomb lattice with a spin-orbit coupling and short-range electron-electron repulsions at half filling, based on the slave-rotor mean-field theory. Besides the conventional QSH phase and a broken-symmetry insulating phase, we find a third phase, a fractionalized quantum spin Hall phase, where the QSH effect arises for fractionalized spinons which carry only spin but not charge. Experimental manifestations of the exotic phase and effects of fluctuations beyond the saddle-point approximation are also discussed.

  • Figure
  • Figure
  • Received 30 July 2008

DOI:https://doi.org/10.1103/PhysRevB.78.125316

©2008 American Physical Society

Authors & Affiliations

Michael W. Young, Sung-Sik Lee, and Catherine Kallin

  • Department of Physics and Astronomy, McMaster University, 1280 Main Street W, Hamilton, Ontario, Canada L8S 4M1

Article Text (Subscription Required)

Click to Expand

References (Subscription Required)

Click to Expand
Issue

Vol. 78, Iss. 12 — 15 September 2008

Reuse & Permissions
Access Options
Author publication services for translation and copyediting assistance advertisement

Authorization Required


×

Images

  • Figure 1
    Figure 1
    Phase diagram in the space of t/t and U/t in a 40×40 lattice with U=0. The weakly interacting phase (small U) has Z0 and the first layer forms the conventional QSH phase while the second layer is in the semimetal (SM) phase with gapless Dirac nodes. The intermediate region has the fractionalized quantum spin Hall (FQSH) phase with Z=0 where chargeless spinons form the QSH phase in the first layer and the gapless spin liquid (SL) phase in the second layer. In both QSH/SM and FQSH/SL phases, the NN and NNN hopping order parameters are nonzero and site independent. The large U region is a dimerized phase where Z=0 and the hopping order parameters along the bold lines have the maximum amplitude and all other bonds have zero amplitude. The solid line represents the second-order transition and the dotted line the first-order transition.Reuse & Permissions
  • Figure 2
    Figure 2
    (Color online) (a) Transverse spin response to an applied external magnetic field in the conventional quantum spin Hall phase. Upon threading a magnetic-flux quantum, a spin up propagates from one edge 1, say, to edge 2 and a spin down propagates from edge 2 to edge 1. (b) The response in the fractionalized quantum spin Hall phase. The external flux does not generate any transverse spin transport because the edge modes are charge neutral spinons.Reuse & Permissions
×

Sign up to receive regular email alerts from Physical Review B

Log In

Cancel
×

Search


Article Lookup

Paste a citation or DOI

Enter a citation
×