Abstract

We propose to apply a modified version of the excitation scheme introduced by Volchkov et al. on bosons experiencing hyperfine state dependent disorder to address the critical state at the mobility edge of the Anderson localization transition, and to observe its intriguing multifractal structure. An optimally designed, spatially focused external radio frequency pulse can be applied to generate transitions to eigenstates in a narrow energy window close to the mobility edge, where critical scaling and multifractality emerge. Alternatively, two-photon laser scanning microscopy is proposed to address individual localized states even close to the transition. The projected image of the cloud is shown to inherit multifractality and to display universal density correlations. Interactions – unavoidably present – are taken into account by solving the Gross-Pitaevskii equations, and their destructive effect on the spectral resolution and the multifractal spectrum is analyzed. Time of flight images of the excited states are predicted to show interference fringes in the localized phase, while they allow one to map equal energy surfaces deep in the metallic phase.

Highlights

  • Anderson localization is one of the most fundamental quantum interference phenomena in disordered quantum systems

  • Indications of multicriticality have been reported in ultrasound experiments[37] but, the universal multifractal spectrum of the critical state has not been observed in these experiments, either[37,43]

  • We carried out detailed large scale Gross-Pitaevskii simulations to investigate selective final state spectroscopy in an interacting disordered two-component Bose condensate

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Summary

Introduction

Anderson localization is one of the most fundamental quantum interference phenomena in disordered quantum systems. We propose to use a thin vertical laser beam with two frequencies to produce two-photon Raman transitions to localized states in a narrow spatial range and at a well-defined energy such that that the excited wave functions do not overlap.

Results
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