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Topological spin models in Rydberg lattices

Abstract:
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 .
Publication status:
Published
Peer review status:
Peer reviewed

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Publisher copy:
10.1007/s00340-016-6596-4

Authors


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Institution:
University of Oxford
Division:
MPLS
Department:
Mathematical Institute
Role:
Author
More by this author
Institution:
University of Oxford
Oxford college:
Keble College
Role:
Author


Publisher:
Springer Verlag
Journal:
Applied Physics B More from this journal
Volume:
123
Issue:
46
Publication date:
2017-01-16
Acceptance date:
2016-11-12
DOI:
EISSN:
1432-0649
ISSN:
0946-2171


Pubs id:
pubs:659315
UUID:
uuid:e9dea66b-1489-4bf9-9fb5-8cd1890332c3
Local pid:
pubs:659315
Source identifiers:
659315
Deposit date:
2016-11-14

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