2016
DOI: 10.1088/1367-2630/18/1/013039
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Can 3D light localization be reached in ‘white paint’?

Abstract: When waves scatter multiple times in 3D random media, a disorder driven phase transition from diffusion to localization may occur (Anderson 1958 Phys. Rev. 109 1492-505; Abrahams et al 1979 Phys. Rev. Lett. 42 673-6). In 'The question of classical localization: a theory of white paint?' Anderson suggested the possibility to observe light localization in TiO 2 samples (Anderson 1985 Phil. Mag. B 52 505-9). We recently claimed the observation of localization effects measuring photon time of flight (ToF) distribu… Show more

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Cited by 96 publications
(101 citation statements)
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References 38 publications
(139 reference statements)
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“…The combination of both methods allows to estimate quantitatively the absorption length: l a 118 µm. Our measurement is in qualitative agreement with transmission time-offlight measurements performed in other TiO 2 samples [29]. An estimation of the transport mean-free path l t is also possible using the relation D = v e l t /3, with v e the energy velocity.…”
Section: (D)]: (I)supporting
confidence: 87%
See 1 more Smart Citation
“…The combination of both methods allows to estimate quantitatively the absorption length: l a 118 µm. Our measurement is in qualitative agreement with transmission time-offlight measurements performed in other TiO 2 samples [29]. An estimation of the transport mean-free path l t is also possible using the relation D = v e l t /3, with v e the energy velocity.…”
Section: (D)]: (I)supporting
confidence: 87%
“…A further step would be to investigate exotic transport phenomena such as super-and sub-diffusion of light [41,42] or, more ambitiously, to provide a direct proof for Anderson localization [43,44]. Past experimental studies of Anderson localization in optics have been ambiguous, due either to absorption effects [45,46] or fluorescence issues [29]. On the contrary, our approach would remove any possible ambiguity.…”
mentioning
confidence: 97%
“…Localization is the rule for large enough 1D and 2D systems, but a genuine, disorder-driven metal-insulator transition, the Anderson transition (AT), occurs in 3D [5,6]. Over the past fifty years, numerous experiments have revealed the delicate intricacies of Anderson localization [7,8,9,10,11,12,13,14].…”
Section: Introductionmentioning
confidence: 99%
“…This idea was indeed supported by the observation of the destruction of the coherent backscattering cone (CBC, which is often seen as the precursor of Anderson localization) in Faraday active multiple scattering samples [4,11]. While optical waves a e-mail: Geoffroy.Aubry@uni-konstanz.de b e-mail: Georg.Maret@uni-konstanz.de still bear to show signs of localization in 3D samples [12,13] Faraday rotation is still a good candidate for a sensitive probe of Anderson localization of light.…”
Section: Introductionmentioning
confidence: 99%