Anderson Localization in the Induced Disorder System
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Abstract
We propose a coherently prepared three-level atomic medium that can provide a flexible disordered scheme for realizing the Anderson localization. Different disorder levels can be attained by modulating the intensity ratio between the two control beams. Due to the real-time tunability, the localization of the signal beam is observable and controllable. The influences of the induced disorder level, atomic density and the initial waist radius of the signal beam on the Anderson localization in the medium are also discussed.
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Fei-Fei Lu, Chun-Fang Wang. Anderson Localization in the Induced Disorder System[J]. Chin. Phys. Lett., 2016, 33(7): 074202. DOI: 10.1088/0256-307X/33/7/074202
Fei-Fei Lu, Chun-Fang Wang. Anderson Localization in the Induced Disorder System[J]. Chin. Phys. Lett., 2016, 33(7): 074202. DOI: 10.1088/0256-307X/33/7/074202
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Fei-Fei Lu, Chun-Fang Wang. Anderson Localization in the Induced Disorder System[J]. Chin. Phys. Lett., 2016, 33(7): 074202. DOI: 10.1088/0256-307X/33/7/074202
Fei-Fei Lu, Chun-Fang Wang. Anderson Localization in the Induced Disorder System[J]. Chin. Phys. Lett., 2016, 33(7): 074202. DOI: 10.1088/0256-307X/33/7/074202
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