Strongly correlated material
Strongly correlated materials are a wide class of compounds that include insulators and electronic materials, and show unusual electronic and magnetic properties, such as metal-insulator transitions, heavy fermion behavior, half-metallicity, and spin-charge separation. The essential feature that defines these materials is that the behavior of their electrons or spinons cannot be described effectively in terms of non-interacting entities. Theoretical models of the electronic structure of strongly correlated materials must include electronic correlation to be accurate. As of recently, the label quantum materials is also used to refer to strongly correlated materials, among others.
Transition metal oxides
Many transition metal oxides belong to this class which may be subdivided according to their behavior, e.g. high-Tc, spintronic materials, multiferroics, Mott insulators, spin Peierls materials, heavy fermion materials, quasi-low-dimensional materials, etc. The single most intensively studied effect is probably high-temperature superconductivity in doped cuprates, e.g. La2−xSrxCuO4. Other ordering or magnetic phenomena and temperature-induced phase transitions in many transition-metal oxides are also gathered under the term "strongly correlated materials."Electronic structures
Typically, strongly correlated materials have incompletely filled d- or f-electron shells with narrow energy bands. One can no longer consider any electron in the material as being in a "sea" of the averaged motion of the others. Each single electron has a complex influence on its neighbors.The term strong correlation refers to behavior of electrons in solids that is not well-described by simple one-electron theories such as the local-density approximation of density-functional theory or Hartree–Fock theory. For instance, the seemingly simple material NiO has a partially filled 3d band and therefore would be expected to be a good conductor. However, strong Coulomb repulsion between d electrons makes NiO instead a wide-band gap insulator. Thus, strongly correlated materials have electronic structures that are neither simply free-electron-like nor completely ionic, but a mixture of both.