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Published on: July 29, 2013
Coherent Backscattering Reveals the Anderson Transition
S Ghosh1,2, D Delande1, C Miniatura2,3,4,5
1Laboratoire Kastler Brossel, UPMC-Sorbonne Universités, CNRS, ENS-PSL Research University, Collège de France, 4 Place Jussieu, 75005 Paris, France.
We developed a finite-time scaling analysis to measure the Anderson transition in 3D random media using coherent backscattering (CBS) peak width. This method accurately determines the mobility edge and critical exponent in experiments with ultracold atoms.
Area of Science:
- Condensed matter physics
- Atomic physics
- Wave propagation in disordered media
Background:
- Anderson localization describes the suppression of wave transport in disordered systems.
- Coherent backscattering (CBS) is a wave phenomenon sensitive to localization effects.
- Characterizing the Anderson transition is crucial for understanding electron and wave transport in disordered materials.
Purpose of the Study:
- To develop a finite-time scaling analysis for the angular width of the coherent backscattering (CBS) peak.
- To apply this analysis to ultracold atoms in optical speckle potentials to study the 3D Anderson transition.
- To demonstrate a method for determining the mobility edge and critical exponent of the Anderson transition.
Main Methods:
- Finite-time scaling analysis of the CBS peak's angular width.
- Experimental realization using ultracold atoms in 3D optical speckle potentials.
- Analysis of the temporal behavior of the CBS width to extract transition parameters.
Main Results:
- An accurate finite-time scaling analysis of the CBS peak angular width was developed.
- The method successfully relates the temporal CBS width to the Anderson transition parameters.
- The mobility edge and critical exponent can be determined from the CBS width's temporal evolution.
Conclusions:
- The developed finite-time scaling analysis provides an accurate method to study the 3D Anderson transition.
- This technique, applied to ultracold atoms, allows for precise determination of critical exponents and mobility edges.
- The method offers a powerful experimental tool for fully characterizing Anderson transitions in disordered systems.
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