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Energy-dissipation anomaly in systems of localized waves
1Service de Physique de l'État Condensé, CEA, CNRS, Université Paris-Saclay, CEA Saclay, 91191 Gif-sur-Yvette, France.
Physical Review. E
|June 17, 2017
Summary
In disordered media, wave power dissipation typically vanishes. However, this study reveals surprisingly finite mean dissipated power in the zero-damping limit, linked to the system's density of states.
Area of Science:
- Wave propagation in disordered systems
- Condensed matter physics
- Statistical mechanics
Background:
- Wave propagation in disordered media often leads to Anderson localization.
- Dissipation is typically expected to decrease with vanishing damping.
- Understanding energy transport and loss in such systems is crucial.
Purpose of the Study:
- To investigate the statistics of dissipated power in a damped, one-dimensional disordered medium.
- To analyze the behavior of dissipated power as damping approaches zero.
- To identify the underlying physical mechanism for anomalous dissipation.
Main Methods:
- Analyzing the power statistics under imposed wave amplitude at one end.
- Investigating the singular limit of vanishing damping coefficient (ν→0).
- Relating the mean dissipated power to the integrated density of states.
Main Results:
- The typical dissipated power vanishes as damping approaches zero due to wave localization.
- A surprising, finite mean dissipated power (anomalous dissipation) is observed in the ν→0 limit.
- This anomalous dissipation is shown to be equal to the integrated density of states of the undamped system.
Conclusions:
- Anomalous dissipation in disordered systems is directly determined by the integrated density of states.
- This finding allows for exact calculations of anomalous dissipation using undamped system properties.
- The developed approach is applicable to various types of disorder and damping coefficients.
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