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1.
Opt Express ; 19(22): 21658-64, 2011 Oct 24.
Article in English | MEDLINE | ID: mdl-22109015

ABSTRACT

Optical coherence tomography (OCT) images are frequently interpreted in terms of layers (for example, of tissue) with the boundary defined by a change in refractive index. Real boundaries are rough compared with the wavelength of light, and in this paper we show that this roughness has to be taken into account in interpreting the images. We give an example of the same OCT image obtained from two quite different objects, one smooth compared to the optical wavelength, and the other rough.

2.
Phys Rev E Stat Nonlin Soft Matter Phys ; 64(5 Pt 2): 056620, 2001 Nov.
Article in English | MEDLINE | ID: mdl-11736129

ABSTRACT

The propagation of a narrow-band signal radiated by a point source in a randomly layered absorbing medium is studied asymptotically in the weak-scattering limit. It is shown that in a disordered stratified medium that is homogeneous on average, a pulse is channelled along the layers in a narrow strip in the vicinity of the source. The space-time distribution of the pulse energy is calculated. Far from the source, the shape of wave packets is universal and independent of the frequency spectrum of the radiated signal. Strong localization effects manifest themselves also as a low-decaying tail of the pulse and a strong time delay in the direction of stratification. The frequency-momentum correlation function in a one-dimensional random medium is calculated.

3.
6.
Phys Rev B Condens Matter ; 53(11): 7413-7416, 1996 Mar 15.
Article in English | MEDLINE | ID: mdl-9982188
8.
Phys Rev Lett ; 101(13): 133901, 2008 Sep 26.
Article in English | MEDLINE | ID: mdl-18851448

ABSTRACT

We study the interaction of Anderson localized states in an open 1D random system by varying the internal structure of the sample. As the frequencies of two states come close, they are transformed into multiply peaked quasiextended modes. Level repulsion is observed experimentally and explained within a model of coupled resonators. The spectral and spatial evolution of the coupled modes is described in terms of the coupling coefficient and Q factors of resonators.

9.
Phys Rev Lett ; 97(24): 243904, 2006 Dec 15.
Article in English | MEDLINE | ID: mdl-17280287

ABSTRACT

We consider, both theoretically and experimentally, the excitation and detection of the localized quasimodes (resonances) in an open dissipative 1D random system. We show that, even though the amplitude of transmission drops dramatically so that it cannot be observed in the presence of small losses, resonances are still clearly exhibited in reflection. Surprisingly, small losses essentially improve conditions for the detection of resonances in reflection as compared with the lossless case. An algorithm is proposed and tested to retrieve sample parameters and resonance characteristics inside the random system exclusively from reflection measurements.

10.
Opt Lett ; 19(18): 1382-4, 1994 Sep 15.
Article in English | MEDLINE | ID: mdl-19855526

ABSTRACT

We found that a slightly rough thin dielectric film polarizes diffusely scattered light. There is a discrete set of angles of incidence and observation for which the intensity of a nonspecular diffuse P-polarized component is significantly greater than that for S polarization.

11.
Opt Lett ; 29(12): 1372-4, 2004 Jun 15.
Article in English | MEDLINE | ID: mdl-15233439

ABSTRACT

Scattering of light from rough dielectric films is studied experimentally. It is shown that the interference pattern of the scattered field depends critically on the power spectrum of the roughness, especially on its long-scale component. When the height of roughness is small compared with the wavelength, the backscattering peak (if it exists) is due to the interference of the singly scattered fields; hence the properties of the backscattered peak are rather unusual. In particular, the width of the peak is determined by the thickness of the film and is independent of the parameters of disorder. The intensity of the peak increases with an increase of the rms height of the surface roughness and becomes independent of the rms when the roughness is of the order of the wavelength.

12.
Opt Lett ; 23(5): 316-8, 1998 Mar 01.
Article in English | MEDLINE | ID: mdl-18084497

ABSTRACT

The scattering of light from a slightly rough surface overlying a reflecting surface is investigated. It is shown that the long-scale component of the roughness spectrum plays a critical role in the scattering patterns obtained. The scattered interference patterns are critically dependent on small variation of the rms height of the long-scale component of the roughness. Conventional perturbation theory is found to be invalid in cases in which interference phenomena in the scattering are of importance. A model is proposed that quantitatively describes the measured angular intensity distributions.

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