Topological spin models in Rydberg lattices

We show that resonant dipole–dipole interactions between Rydberg atoms in a triangular lattice can give rise to artificial magnetic fields for spin excitations. We consider the coherent dipole–dipole coupling between np and ns Rydberg states and derive an effective spin-1/2 Hamiltonian for the np ex...

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Main Authors: Kiffner, M, O’Brien, E, Jaksch, D
Format: Journal article
Published: Springer Verlag 2017
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author Kiffner, M
O’Brien, E
Jaksch, D
author_facet Kiffner, M
O’Brien, E
Jaksch, D
author_sort Kiffner, M
collection OXFORD
description We show that resonant dipole–dipole interactions between Rydberg atoms in a triangular lattice can give rise to artificial magnetic fields for spin excitations. We consider the coherent dipole–dipole coupling between np and ns Rydberg states and derive an effective spin-1/2 Hamiltonian for the np excitations. By breaking time-reversal symmetry via external fields, we engineer complex hopping amplitudes for transitions between two rectangular sub-lattices. The phase of these hopping amplitudes depends on the direction of the hop. This gives rise to a staggered, artificial magnetic field which induces non-trivial topological effects. We calculate the single-particle band structure and investigate its Chern numbers as a function of the lattice parameters and the detuning between the two sub-lattices. We identify extended parameter regimes where the Chern number of the lowest band is C=1C=1 or C=2C=2 .
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spelling oxford-uuid:e9dea66b-1489-4bf9-9fb5-8cd1890332c32022-03-27T10:57:24ZTopological spin models in Rydberg latticesJournal articlehttp://purl.org/coar/resource_type/c_dcae04bcuuid:e9dea66b-1489-4bf9-9fb5-8cd1890332c3Symplectic Elements at OxfordSpringer Verlag2017Kiffner, MO’Brien, EJaksch, DWe show that resonant dipole–dipole interactions between Rydberg atoms in a triangular lattice can give rise to artificial magnetic fields for spin excitations. We consider the coherent dipole–dipole coupling between np and ns Rydberg states and derive an effective spin-1/2 Hamiltonian for the np excitations. By breaking time-reversal symmetry via external fields, we engineer complex hopping amplitudes for transitions between two rectangular sub-lattices. The phase of these hopping amplitudes depends on the direction of the hop. This gives rise to a staggered, artificial magnetic field which induces non-trivial topological effects. We calculate the single-particle band structure and investigate its Chern numbers as a function of the lattice parameters and the detuning between the two sub-lattices. We identify extended parameter regimes where the Chern number of the lowest band is C=1C=1 or C=2C=2 .
spellingShingle Kiffner, M
O’Brien, E
Jaksch, D
Topological spin models in Rydberg lattices
title Topological spin models in Rydberg lattices
title_full Topological spin models in Rydberg lattices
title_fullStr Topological spin models in Rydberg lattices
title_full_unstemmed Topological spin models in Rydberg lattices
title_short Topological spin models in Rydberg lattices
title_sort topological spin models in rydberg lattices
work_keys_str_mv AT kiffnerm topologicalspinmodelsinrydberglattices
AT obriene topologicalspinmodelsinrydberglattices
AT jakschd topologicalspinmodelsinrydberglattices