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Universal Anderson localization in one-dimensional unitary maps.

Ihor Vakulchyk1,2, Sergej Flach1,2

  • 1Center for Theoretical Physics of Complex Systems, Institute for Basic Science (IBS), Daejeon 34126, Republic of Korea.

Chaos (Woodbury, N.Y.)
|December 7, 2023
PubMed
Summary
This summary is machine-generated.

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We discovered universal Anderson localization in discrete-time quantum maps. Strong disorder leads to exponentially localized eigenstates with a single, tunable localization length, offering new insights into quantum chaos.

Area of Science:

  • Quantum physics
  • Condensed matter physics
  • Disordered systems

Background:

  • Anderson localization describes the suppression of wave function propagation in disordered systems.
  • Discrete-time quantum maps offer a simplified yet powerful model for studying quantum dynamics.

Purpose of the Study:

  • To investigate Anderson localization in one-dimensional discrete-time quantum maps.
  • To analyze the impact of disorder on quantum dynamics and eigenstate localization.
  • To develop an exact theory for the localization length.

Main Methods:

  • Studying Anderson localization in discrete-time quantum map dynamics.
  • Introducing nearest-neighbor hopping strength θ and quasienergies on the unit circle.
  • Analyzing the effect of strong disorder in a local phase field.

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Main Results:

  • Demonstrated uniform spectrum gaplessly occupying the unit circle under strong disorder.
  • Observed that all resulting eigenstates are exponentially localized.
  • Found that Anderson localization is universal, with all eigenstates sharing the same localization length (Lloc).

Conclusions:

  • Developed an exact theory for calculating the localization length: 1/Lloc=|ln(|sin(θ)|)|.
  • Showcased that the localization length is tunable from zero to infinity by varying the hopping strength θ.
  • Confirmed universal Anderson localization in this quantum system.