Key role of the moire potential for the quasi-condensation of interlayer excitons in van der Waals heterostructures
arXiv:2009.12943 · doi:10.1103/PhysRevB.103.L041406
Abstract
Interlayer excitons confined in bilayer heterostructures of transition metal dichalcogenides (TMDs) offer a promising route to implement two-dimensional dipolar superfluids. Here, we study the experimental conditions necessary for the realisation of such collective state. Particularly, we show that the moire potential inherent to TMD bilayers yields an exponential increase of the excitons effective mass. To allow for exciton superfluidity at sizeable temperatures it is then necessary to intercalate a high- dielectric between the monolayers confining electrons and holes. Thus the moire lattice depth is sufficiently weak for a superfluid phase to theoretically emerge below a critical temperature of around 10 K. Importantly, for realistic experimental parameters interlayer excitons quasi-condense in a state with finite momentum, so that the superfluid is optically inactive and flows spontaneously.
6 pages, 4 figures
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- Extended spatial coherence of interlayer excitons in MoSe/WSe heterobilayers
- Bosonic Delocalization of Dipolar Moiré Excitons
- Exciton-phonon-scattering: A competition between bosonic and fermionic nature of bound electron-hole pairs
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- Quantum anomalous Hall effect and electric-field-induced topological phase transition in AB-stacked MoTe/WSe moiré heterobilayers
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- Confined-state physics and signs of fermionization of moiré excitons in WSe/MoSe heterobilayers
- Moiré exciton condensate: nonlinear Dirac point, broken-symmetry Bloch waves and unusual optical selection rules
- Fermionic vs. bosonic thermalization in the phonon-driven exciton dynamics: An analytic dimensionality study
- Laterally Extended States of Interlayer Excitons in Reconstructed MoSe/WSe Heterostructures
- Non-local interactions and supersolidity of moiré excitons