Condensed Matter Physics, 2019, vol. 22, No. 1, 13701
DOI:10.5488/CMP.22.13701
arXiv:1808.03560
Title:
Emergence of topological Mott insulators in proximity of quadratic band touching points
Author(s):
 
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I. Mandal
(Laboratory of Atomic And Solid State Physics, Cornell University, Ithaca, NY 14853, USA)
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S. Gemsheim
(Fakultät Physik, Technische Universität Dresden, 01069 Dresden, Germany)
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Recently, the field of strongly correlated electrons has begun an intense search for a correlation induced topological insulating phase. An example is the quadratic band touching point
which arises in a checkerboard lattice at half-filling, and in the presence of interactions gives rise to topological Mott insulators. In this work, we perform a mean-field theory
computation to show that such a system shows instability to topological insulating phases even away from half-filling (chemical potential μ = 0). The interaction parameters
consist of on-site repulsion (U), nearest-neighbour repulsion (V), and a next-nearest-neighbour correlated hopping (tc). The tc interaction
originates from strong Coulomb repulsion. By tuning the values of these parameters, we obtain a desired topological phase that spans the area around (V = 0, μ = 0), extending to
regions with (V > 0, μ = 0) and (V > 0, μ > 0). This extends the realm of current experimental efforts to find these topological phases.
Key words:
checkerboard, quadratic band touching points, topology, Mott insulator, d-density wave
PACS:
73.43.-f, 73.43.Nq, 71.10.Fd
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