First proposed in 1958 by American theoretical physicist Philip W. Anderson, Anderson localization describes the unique behavior of electrons in disordered materials[1]. These electrons become trapped, or localized, in materials characterized by random abnormalities, marking a significant moment in contemporary condensed matter physics. This theory applies to both quantum and classical mechanics.
In the classical realm, we'd envision a particle bouncing around like a pinball through a maze, scattered by defects. However, in quantum physics, the wave-like identity of a particle becomes incredibly complex, forcing the electron to stop and transforming the material into an insulator.
This phenomenon also appears to occur with the electromagnetic waves that compose light as they scatter through certain substances, at least in one or two dimensions. Until recently, however, it remained unclear whether this physics holds in three dimensions.
Thanks to significant advances in calculation software and numerical simulations, this long-standing mystery has finally been solved. This breakthrough in quantum physics opens up new avenues for research and could potentially have far-reaching implications for our understanding of the universe.
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