3) Polariton and topological matter

Topology describes properties of a physical system that remain unaffected by distortion. The most straightforward example is the “genus”: the number of holes of a closed surface. For instance, a mug and a donut both have a hole, they both possess the same topological invariant (genus=1) and they can be transformed into each other via smooth deformations.

In solid state materials we can apply the same idea: we can define a topological invariant related to the properties of the electronic bands. Even though the bands and electronic eigenfunctions change when we deform the material, the topological invariant remains the same, and the only way to change it is by closing the gap between the bands. This has a very important consequence: when two materials with bands with different topological invariants are brought together, the gap needs to close exactly at the frontier between the materials. This means that an interface mode appears in the middle of the gap. As the existence of this “edge” mode is related to the topological properties of the bulk, it will always be there, no matter the shape of the region between the two materials. These concepts have explained the chiral edge transport in the quantum Hall effect, which is robust to disorder in the Hall bar, or the emergence of topological insulators that conduct only on their surface.

Implementing these ideas in photonics is promising route towards photonic devices with transport immune to scattering. Namely, photons in a topological lattice are able to travel on the edge of the lattice no matter its shape. In the past few years, we have implemented lattices of coupled polariton resonators with various topological properties. In particular, we have addressed the physics of the honeycomb lattice, the Su-Schrieffer-Heeger (SSH) lattice, and we have demonstrated the existence of edge states connected to the properties of the bulk. In the SSH lattice, we have obtained the first laser in a topological mode, and we have shown that it is robust to local perturbations of the photonic potential (see focus here). Our projects include studying nonlinear topological properties, novel Floquet phases and high-order topological insulators.

The group is part of the team “Dysco” of the PhLAM laboratory, and works in strong collaboration with the group of Jacqueline Bloch at Center for Nanosciences and Nanotechnologies.

More information: http://honeypol.eu/

Group members

Alberto Amo (CNRS researcher)

Omar Jamadi (post-doc)

Bastian Real (PhD student)

Corentin Lechevalier (PhD student)

Krzysztof Sawicki (visiting PhD student)

Cécilia Ouarkoub (master student)

Selected publications:

  • Topological photonics
    T. Ozawa, H. M. Price, A. Amo, N. Goldman, M. Hafezi, L. Lu, M. Rechtsman, D. Schuster, J. Simon, O. Zilberberg, I. Carusotto, Rev. Mod. Phys. 91, 15006 (2019). [PDF]

  • Type-III and tilted Dirac cones emerging from flat bands in photonic orbital graphene
    M. Milićević, G. Montambaux, T. Ozawa, O. Jamadi, B. real, I. Sagnes, A. Lemaître, L. Le Gratiet, A. Harouri, J. Bloch, A. Amo, Phys. Rev. X 9, 31010 (2019) [PDF]

  • Lasing in topological edge states of a 1D lattice
    P. St-Jean, V. Goblot, E. Galopin, A. Lemaître, T. Ozawa, L. Le Gratiet, I.Sagnes, J. Bloch, A. Amo, Nat. Photon. 11, 651 (2017). [PDF] [PDF Suppl.see focus

  • Exploring topological edge states in photonic quasicrystals
    F. Baboux, E. Levy, A. Lemaître, C. Gomez, E. Galopin, L. Le Gratiet, I. Sagnes, A. Amo, J. Bloch, and E. Akkermans, , Phys. Rev. B 95, 161114(R) (2017). [PDF] [PDF Suppl.]

  • Orbital edge states in a photonic honeycomb lattice
    M. Milićević, T. Ozawa, G. Montambaux, I. Carusotto, E. Galopin, A. Lemaître, L. Le Gratiet, I. Sagnes, J. Bloch, and A. Amo, Phys. Rev Lett. 118, 107403 (2017). [PDF] [PDF Suppl.]

  • Spin-Orbit Coupling for Photons and Polaritons in Microstructures
    V. G. Sala, D. D. Solnyshkov, I. Carusotto, T. Jacqmin, A. Lemaître, H. Terças, A. Nalitov, M. Abbarchi, E. Galopin, I. Sagnes, J. Bloch, G. Malpuech, and A. Amo, Phys. Rev. X 5, 011034 (2015). [PDF] [PDF Suppl.]

  • Direct observation of Dirac cones and a flatband in a honeycomb lattice for polaritons
    T. Jacqmin, I. Carusotto, I. Sagnes, M. Abbarchi, D. Solnyshkov, G. Malpuech, E. Galopin, A. Lemaître, J. Bloch, A. Amo, , Phys. Rev. Lett. 112, 116402 (2014). [PDF] [PDF Suppl.]