Wing-Ho Ko
Massachusetts Institute of Technology
Network
Latest external collaboration on country level. Dive into details by clicking on the dots.
Publication
Featured researches published by Wing-Ho Ko.
Physical Review B | 2009
Wing-Ho Ko; Patrick A. Lee; Xiao-Gang Wen
A Chern-Simons theory for the doped spin-1/2 kagome system is constructed, from which it is shown that the system is an exotic superconductor that breaks time-reversal symmetry. It is also shown that the system carries minimal vortices of flux
Physical Review B | 2007
Wing-Ho Ko; Cody P. Nave; Patrick A. Lee
hc/4e
Physical Review Letters | 2009
Ying Ran; Wing-Ho Ko; Patrick A. Lee; Xiao-Gang Wen
(as opposed to the usual
Physical Review B | 2011
Wing-Ho Ko; Patrick A. Lee
hc/2e
Physical Review B | 2011
Wing-Ho Ko; Patrick A. Lee
in conventional superconductors) and contains fractional quasiparticles (including fermionic quasiparticles with semionic mutual statistics and spin-1/2 quasiparticles with bosonic self-statistics) in addition to the usual spin-1/2 fermionic Bogoliubov quasiparticles. Two Chern-Simons theories\char22{}one with an auxiliary gauge field kept and one with the auxiliary field and a redundant matter field directly eliminated\char22{}are presented and shown to be consistent with each other.
Physical Review B | 2010
Wing-Ho Ko; Zheng-Xin Liu; Tai Kai Ng; Patrick A. Lee
The generalization of the Gutzwiller approximation to inhomogeneous systems is considered, with extra spin-and-site-dependent fugacity factors included. It is found that the inclusion of fugacity factors reconciles the seemingly contradictory choices of Gutzwiller factors used in the literature. Moreover, from the derivation of the Gutzwiller factors, it is shown that the Gutzwiller approximation breaks the rotational symmetry of the trial wave functions and that different components of the spin-spin interaction need to be renormalized differently under the approximation. Various schemes to restore the rotational symmetry are discussed and are compared with results from variational Monte Carlo calculations for the two-dimensional square-lattice antiferromagnet. Results along different paths within the full parameter space, which correspond to different choices of fugacity factors in the literature, are also compared.
Physical Review B | 2013
Wing-Ho Ko; Leon Balents; Jeffrey G. Rau; Hong-Chen Jiang
The Dirac spin liquid was proposed to be the ground state of the spin-1/2 kagomé antiferromagnets. In a magnetic field B, we show that the state with Fermi pocket is unstable to the Landau level (LL) state. The LL state breaks the spin rotation around the axis of the magnetic field. We find that the LL state has an in-plane 120 degrees q=0 magnetization M which scales with the external field M approximately B;{alpha}, where alpha is a universal number of the Dirac spin liquid. We discuss the related experimental implications which can be used to detect the possible Dirac spin liquid phase in herbertsmithite ZnCu3(OH)6Cl2.
Bulletin of the American Physical Society | 2013
Wing-Ho Ko; Hong-Chen Jiang; Jeffrey G. Rau; Leon Balents
Motivated by the debate of spin-density-wave (SDW) versus local-moment (LM) picture in the iron-based superconducting (FeSC) materials, we consider a two-band orbital-symmetric Hubbard model in which there is robust Fermi surface nesting at
Archive | 2011
Wing-Ho Ko; Patrick A. Lee
(\pi,0)
Archive | 2008
Wing-Ho Ko; Patrick A. Lee; Xiao-Gang Wen
. We obtain the phase diagram of such system by a mean-field slave-rotor approach, in which the Fermi surface nesting and the SDW order are explicitly taken into account via a natural separation of scale between the Hunds coupling and the Coulomb interaction. We find that for a sizable range of Hunds coupling the Mott transition acquires a strong first-order character, but there also exists a small range of stronger Hunds coupling in which an enhancement of magnetization can be observed on the SDW side. We interpret the former scenario as one in which a sharp distinction can be drawn between LM and the SDW picture, and the latter scenario as one in which signs of LM physics begin to develop in the metallic phase. It is tempting to suggest that some FeSC materials are in the vicinity of the latter scenario.