2016
DOI: 10.1103/physreva.93.013827
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Momentum-space Landau levels in driven-dissipative cavity arrays

Abstract: We theoretically study the driven-dissipative Harper-Hofstadter model on a 2D square lattice in the presence of a weak harmonic trap. Without pumping and loss, the eigenstates of this system can be understood, in certain limits, as momentum-space toroidal Landau levels, where the Berry curvature, a geometrical property of an energy band, acts like a momentum-space magnetic field. We show that key features of these eigenstates can be observed in the steady-state of the driven-dissipative system under a monochro… Show more

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Cited by 9 publications
(10 citation statements)
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“…Looking to the future, our proposal can be naturally extended to include a confining external potential, leading to novel oscillation features associated with analogue momentum-space magnetism [60][61][62]. Beyond the small oscillation regime considered so far, systems of pendula also show nonlinear effects such as amplitude-dependent oscillation frequencies.…”
Section: Discussionmentioning
confidence: 94%
“…Looking to the future, our proposal can be naturally extended to include a confining external potential, leading to novel oscillation features associated with analogue momentum-space magnetism [60][61][62]. Beyond the small oscillation regime considered so far, systems of pendula also show nonlinear effects such as amplitude-dependent oscillation frequencies.…”
Section: Discussionmentioning
confidence: 94%
“…In physics, there is a powerful duality between position and momentum, such that a physical system can be equivalently described in either position space or momentum space. If the roles of position and momentum are reversed, this can lead to momentum-space topological physics, ranging from momentum-space lattices 70,71 , to momentum-space Landau levels 72,73 , and momentumspace integer 74 and fractional 75 quantum Hall effects. In the context of synthetic dimensions, the positionmomentum duality is reflected in a re-interpretation of a discrete set of free-particle momentum states as the set of lattice sites 38,39,43 .…”
Section: B Momentum Statesmentioning
confidence: 99%
“…Thus, ψ 1,p is the only nonzero component of the wave function. Its time evolution obeys i∂ t ψ 1,p (t) = H M ψ 1,p (t), with an effective Hamiltonian [16,17]…”
Section: Effective Momentum-space Hamiltonianmentioning
confidence: 99%