Abstract

We propose 1D and 2D lattice wave functions constructed from the SU(n)1 Wess–Zumino–Witten (WZW) model and derive their parent Hamiltonians. When all spins in the lattice transform under SU(n) fundamental representations, we obtain a two-body Hamiltonian in 1D, including the SU(n) Haldane–Shastry model as a special case. In 2D, we show that the wave function converges to a class of Halperin's multilayer fractional quantum Hall states and belongs to chiral spin liquids. Our result reveals a hidden SU(n) symmetry for this class of Halperin states. When the spins sit on bipartite lattices with alternating fundamental and conjugate representations, we provide numerical evidence that the state in 1D exhibits quantum criticality deviating from the expected behaviors of the SU(n)1 WZW model, while in 2D they are chiral spin liquids being consistent with the prediction of the SU(n)1 WZW model.

Highlights

  • SU(n) quantum antiferromagnets have been an extensively studied class of strongly correlated systems in condensed matter

  • In 2D, we find that, on an infinite plane, the wave function converges to a special class of Halperin states that appeared in the context of the multilayer fractional quantum Hall (FQH) effect

  • In summary, we have constructed a family of spin wave functions with SU(n) symmetry from conformal field theories (CFTs), and we have used the CFT properties of the states to derive parent Hamiltonians in both 1D and 2D

Read more

Summary

INTRODUCTION

SU(n) quantum antiferromagnets have been an extensively studied class of strongly correlated systems in condensed matter. Apart from that, for rational CFTs, the existence of null fields allows to derive a (long-range) parent Hamiltonian [56] Following this approach, wave functions have been constructed for the SU(2)k and SO(n) WZW models [56, 59], as well as c = 1 free boson CFTs at particular rational radii [60]. We construct spin wave functions using the SU(n) WZW model and derive parent Hamiltonians of these states in 1D and 2D.

Wave functions
Null vectors
Decoupling equations
Vertex operator representation
Wave functions in the hardcore boson basis
Jastrow wave functions for the uniform 1D lattice
Numerical results
PARENT HAMILTONIANS FOR THE STATES FROM THE FUNDAMENTAL REPRESENTATION
Exchange form of the parent Hamiltonian
Identifying CFT from finite-size spectra
CONCLUSION
VIII. ACKNOWLEDGMENT
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call