
A condition where light remains trapped over a wide range of incidence angles.A flat band is a special energy band in a material's electronic structure where the energy does not depend on the momentum of the electron. In ordinary materials, electrons with different momenta have different energies, forming a curved band. In a flat band, all electrons have the same energy regardless of how fast they move, which means they have an infinite effective mass and are effectively localized. This extreme condition leads to strong electron-electron interactions, as the kinetic energy is quenched, and can give rise to exotic quantum phases such as superconductivity and magnetism.
The concept of flat bands was theoretically predicted in the 1990s, but it gained prominence in 2018 when Pablo Jarillo-Herrero's group at MIT discovered that twisting two layers of graphene at a 'magic angle' of about 1.1 degrees creates flat bands that exhibit superconductivity. This sparked a surge of research into twistronics and flat-band physics.
Flat bands arise from destructive interference of electron wave functions in certain lattice geometries, such as the Kagome lattice or Lieb lattice. In these structures, the hopping of electrons between sites can cancel out for certain states, trapping them in place. The flatness of the band is a result of the lattice symmetry, and it can be tuned by applying strain or magnetic fields. When the band is partially filled, the electrons' Coulomb repulsion dominates over their kinetic energy, leading to correlated states that are not described by simple band theory.
Flat bands are a platform for studying strongly correlated electron systems and for designing new superconductors, quantum spin liquids, and devices for quantum computing.
The 'magic angle' in twisted bilayer graphene is so precise that a deviation of just 0.1 degrees destroys the flat band and the associated superconductivity.









