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Chiral polaron formation on the edge of topological quantum matter
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Immersing a mobile impurity in a quantum many-body environment can reveal fundamental properties of the background medium, hence providing a powerful probe of quantum matter. This approach is particularly intriguing when considering media with exotic properties, such as strongly-correlated phases and topological states of matter. In this work, we study the dressing of a mobile impurity interacting with a chiral mode, as provided by the edge of topological quantum matter. The resulting ''chiral polaron'' is characterized by an asymmetric spectral function, which reflects the chirality and group velocity of the topological edge mode and the drag experienced by the mobile impurity. We first build our theoretical understanding from an effective one-dimensional chiral model, which captures the hallmark signatures of the chiral polaron. We then demonstrate how this simple picture extends to realistic models of integer and fractional Chern insulator states, by adapting tensor-network methods to polaron spectroscopy. Injecting mobile impurities on the edge of topological quantum matter is shown to be a powerful tool to probe exotic edge properties, particularly suitable for cold-atom experiments.
Forward citations
Cited by 3 Pith papers
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Lattice Bose polarons at strong coupling and quantum criticality
A strong-coupling ladder theory for an impurity in a Bose-Hubbard bath near the MI-SF critical point predicts a cusp and a new polaron branch, with energies in good agreement with quantum Monte Carlo.
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Quantum impurities in finite-temperature Bose gases: Detecting vortex proliferation across the BKT and BEC transitions
A repulsively coupled impurity in a finite-temperature Bose gas develops an attractive spectral line when it binds to vortices and density holes, providing a potential local probe of vortex proliferation across the BK...
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Polaronic dressing of bound states
Polaronic dressing from a Bose-Einstein condensate destroys a loosely bound dimer of two impurity atoms while a tightly bound dimer survives, with the crossover set by the ratio of dimer binding energy to polaron energy.
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