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Localization transition in incommensurate non-Hermitian systems
1Department of Physics and School of Computational Sciences, George Mason University, Fairfax, Virginia 22030, USA.
Summary
Researchers discovered a localization transition in one-dimensional lattice models with complex potentials. This transition from extended to localized states is marked by changes in the complex eigenspectrum and is crucial for understanding quantum systems.
Area of Science:
- Condensed matter physics
- Quantum mechanics
- Mathematical physics
Background:
- One-dimensional lattice models are fundamental in condensed matter physics.
- Complex potentials introduce unique quantum phenomena.
- Localization transitions alter the behavior of quantum states.
Purpose of the Study:
- To investigate the localization transition in a specific class of 1D lattice models.
- To analyze the role of incommensurate complex potentials in quantum localization.
- To characterize the behavior of the complex eigenspectrum during the transition.
Main Methods:
- Analysis of a one-dimensional lattice model with a specific complex potential: V(theta)=2[lambda(r) cos(theta)+i(lambda)(i) sin(theta)].
- Examination of the complex eigenspectrum to identify signatures of localization.
- Study of the measure of states with real eigenenergies in different phases.
Main Results:
- A localization transition occurs at the critical point |lambda(r)| + |lambda(i)| = 1.
- The transition is characterized by the measure of real eigenenergy states vanishing in the localized phase.
- Extended states exhibit real spectra when |lambda(r)| >= |lambda(i)|.
- The imaginary part of the spectrum is boundary-condition dependent only near the localization onset.
Conclusions:
- The studied 1D lattice models exhibit a clear localization transition driven by complex potentials.
- The complex eigenspectrum serves as a robust indicator of extended versus localized states.
- The findings offer insights into quantum transport and Anderson localization in complex systems.