Non-local interactions induce quantum-geometry-driven spin loop currents that lift degeneracies and open a full gap, realizing a topological Kondo insulator in MoTe2/WSe2 at ν=2.
Korm´ anyos, G
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Mass imbalance and Coulomb strength control a BCS-BEC crossover in polaritonic condensates, with semiconductors favoring BEC-like excitonic states at low density and semimetals favoring BCS pairing except at strong interactions and large imbalance.
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Topological Kondo Insulator from Spin Loop Currents
Non-local interactions induce quantum-geometry-driven spin loop currents that lift degeneracies and open a full gap, realizing a topological Kondo insulator in MoTe2/WSe2 at ν=2.
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BCS-BEC crossover of polaritonic condensates in mass-imbalanced semimetal/semiconductor microcavities
Mass imbalance and Coulomb strength control a BCS-BEC crossover in polaritonic condensates, with semiconductors favoring BEC-like excitonic states at low density and semimetals favoring BCS pairing except at strong interactions and large imbalance.