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  2. Mott insulator - Wikipedia

    en.wikipedia.org/wiki/Mott_insulator

    In general, Mott insulators occur when the repulsive Coulomb potential U is large enough to create an energy gap. One of the simplest theories of Mott insulators is the 1963 Hubbard model. The crossover from a metal to a Mott insulator as U is increased, can be predicted within the so-called dynamical mean field theory.

  3. Neuromorphic computing - Wikipedia

    en.wikipedia.org/wiki/Neuromorphic_computing

    Neuromorphic quantum computing [37] (abbreviated as 'n.quantum computing') is an unconventional computing type of computing that uses neuromorphic computing to perform quantum operations. [ 38 ] [ 39 ] It was suggested that quantum algorithms , which are algorithms that run on a realistic model of quantum computation , can be computed equally ...

  4. Nevill Mott - Wikipedia

    en.wikipedia.org/wiki/Neville_Mott

    Sir Nevill Francis Mott (30 September 1905 – 8 August 1996) was a British physicist who won the Nobel Prize for Physics in 1977 for his work on the electronic structure of magnetic and disordered systems, especially amorphous semiconductors.

  5. Carver Mead - Wikipedia

    en.wikipedia.org/wiki/Carver_Mead

    Mead's contributions have arisen from the application of basic physics to the development of electronic devices, often in novel ways. During the 1960s, he carried out systematic investigations into the energy behavior of electrons in insulators and semiconductors, developing a deep understanding of electron tunneling, barrier behavior and hot electron transport. [13]

  6. Metal–insulator transition - Wikipedia

    en.wikipedia.org/wiki/Metal–insulator_transition

    Since then, these materials as well as others exhibiting a transition between a metal and an insulator have been extensively studied, e.g. by Sir Nevill Mott, after whom the insulating state is named Mott insulator. The first metal-insulator transition to be found was the Verwey transition of magnetite in the 1940s. [3]

  7. Bose–Hubbard model - Wikipedia

    en.wikipedia.org/wiki/Bose–Hubbard_model

    At zero temperature, the Bose–Hubbard model (in the absence of disorder) is in either a Mott insulating state at small /, or in a superfluid state at large /. [8] The Mott insulating phases are characterized by integer boson densities, by the existence of an energy gap for particle-hole excitations, and by zero compressibility .

  8. Strongly correlated material - Wikipedia

    en.wikipedia.org/wiki/Strongly_correlated_material

    The perovskite structure of BSCCO, a high-temperature superconductor and a strongly correlated material.. Strongly correlated materials are a wide class of compounds that include insulators and electronic materials, and show unusual (often technologically useful) electronic and magnetic properties, such as metal-insulator transitions, heavy fermion behavior, half-metallicity, and spin-charge ...

  9. Exciton - Wikipedia

    en.wikipedia.org/wiki/Exciton

    An exciton is a bound state of an electron and an electron hole which are attracted to each other by the electrostatic Coulomb force resulting from their opposite charges. It is an electrically neutral quasiparticle regarded as an elementary excitation primarily in condensed matter, such as insulators, semiconductors, some metals, and in some liquids.