nLab Anderson localization

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Context

Solid state physics

Quantum systems

quantum logic


quantum physics


quantum probability theoryobservables and states


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quantum computing

Contents

Idea

In solid state physics, Anderson localization is the phenomenon that quantum particles may localize in disordered media, meaning that instead of propagating freely they get stuck at certain positions. For electrons in a crystal this means that as the density of impurities becomes large, the crystal may turn from a conductor (where electrons move freely) to an insulator, then called an Anderson insulator.

Anderson localization is a quantum mechanical phenomenon in stark contrast to the situation in classical physics: For the motion of classical bouncing Billiard balls, the presence of “bumpers” (impurities) in their path will make their motion diffuse instead of localize. But for quanta described by wave mechanics the impurities tend to lead to destructive quantum interference of their wavefunction with itself, thus resulting in the localization phenomenon.

References

The original article:

and its modern develoment:

Early experimental observation:

  • Melvin Cutler, N. F. Mott: Observation of Anderson Localization in an Electron Gas, Phys. Rev. 181 (1969) 1336 [doi:10.1103/PhysRev.181.1336]

Review:

See also:

Mathematical discussion:

Further discussion:

  • Tobias Brandes, S. Kettemann (eds.): Anderson Localization and Its Ramifications – Disorder, Phase Coherence, and Electron Correlations, Lecture Notes in Physics 630, Springer (2003) [doi:10.1007/b13139]

  • Marcel Filoche, Svitlana Mayboroda: Universal mechanism for Anderson and weak localization, PNAS 109 37 (2012) 14761-14766 [doi:10.1073/pnas.1120432109]

Last revised on January 19, 2026 at 14:02:05. See the history of this page for a list of all contributions to it.