Linking topological features of the Hofstadter model to optical diffraction figures

In two, three and even four spatial dimensions, the transverse responses experienced by a charged particle on a lattice in a uniform magnetic field are fully controlled by topological invariants called Chern numbers, which characterize the energy bands of the underlying Hofstadter Hamiltonian. These...

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Detalles Bibliográficos
Autores: Di Colandrea, Francesco, D'Errico, Alessio, Maffei, Maria, Price, Hannah M, Lewenstein, Maciej, Marrucci, Lorenzo, Cardano, Filippo, Dauphin, Alexandre, Massignan, Pietro Alberto|||0000-0003-1545-792X
Tipo de recurso: artículo
Fecha de publicación:2022
País:España
Institución:Universitat Politècnica de Catalunya (UPC)
Repositorio:UPCommons. Portal del coneixement obert de la UPC
Idioma:inglés
OAI Identifier:oai:upcommons.upc.edu:2117/388484
Acceso en línea:https://hdl.handle.net/2117/388484
https://dx.doi.org/10.1088/1367-2630/ac4126
Access Level:acceso abierto
Palabra clave:Optics
Topological physics
Hofstadter model
Quantum Hall effect
Òptica no lineal
Àrees temàtiques de la UPC::Ciències de la visió::Òptica física::Òptica fisiològica
Descripción
Sumario:In two, three and even four spatial dimensions, the transverse responses experienced by a charged particle on a lattice in a uniform magnetic field are fully controlled by topological invariants called Chern numbers, which characterize the energy bands of the underlying Hofstadter Hamiltonian. These remarkable features, solely arising from the magnetic translational symmetry, are captured by Diophantine equations which relate the fraction of occupied states, the magnetic flux and the Chern numbers of the system bands. Here we investigate the close analogy between the topological properties of Hofstadter Hamiltonians and the diffraction figures resulting from optical gratings. In particular, we show that there is a one-to-one relation between the above mentioned Diophantine equation and the Bragg condition determining the far-field positions of the optical diffraction peaks. As an interesting consequence of this mapping, we discuss how the robustness of diffraction figures to structural disorder in the grating is a direct analogue of the robustness of transverse conductance in the quantum Hall effect.