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1.
Phys Rev E Stat Nonlin Soft Matter Phys ; 73(3 Pt 2): 036220, 2006 Mar.
Artigo em Inglês | MEDLINE | ID: mdl-16605644

RESUMO

A linear stability analysis is derived in self-imaging cavities for which the conditions for large Fresnel number are stated. In cases of both Fabry-Pérot and ring cavities a Hopf bifurcation is predicted at finite transverse wave number. The self-imaging Fabry-Pérot resonator operates as a longitudinal multimode cavity that invalidates the mean-field model. Above the bifurcation threshold, either vortex lattices, spirals, or targets occur, depending on the Fresnel number, the input intensity, and the mistunings. The time and spatial characteristics have different scales in the case of a self-imaging ring cavity, but the same sort of patterns are reported.

2.
Phys Rev E Stat Nonlin Soft Matter Phys ; 67(6 Pt 2): 066207, 2003 Jun.
Artigo em Inglês | MEDLINE | ID: mdl-16241326

RESUMO

The formation of transverse patterns in a triply resonant optical parametric oscillator is studied both numerically and analytically for a spherical cavity close to confocality. While the pump profile is Gaussian, the signal and idler intensities may be made of many rings, either stationary or time dependent. The mode selection and the time dependence are understood with the help of the linear stability analysis. It might explain observations reported for a quasiconfocal cavity with a KTP crystal.

3.
Phys Rev E Stat Nonlin Soft Matter Phys ; 66(2 Pt 2): 026203, 2002 Aug.
Artigo em Inglês | MEDLINE | ID: mdl-12241263

RESUMO

Labyrinthine structures often appear as the final steady state of pattern forming systems. Being disordered, they exhibit the same kind of short range positional order as the Newell-Pomeau turbulent crystal. Labyrinths can be seen as a limit case of the texture of disordered rolls with a coherence length of the same order as the wavelength. In the various two-dimensional model equations we looked at, labyrinths and parallel rolls are steady states for the same parameters, their occurrence depending on the initial conditions. Comparing the stability of these two structures, we find that in variational models their energy is very close, rolls always being more stable than labyrinths. For the nonvariational model we propose a numerical experiment which displays a well defined bifurcation from parallel rolls to labyrinths as the more stable state.

4.
Opt Lett ; 25(7): 487-9, 2000 Apr 01.
Artigo em Inglês | MEDLINE | ID: mdl-18064088

RESUMO

We study the dynamics of the formation of circular domain walls, which are large-intensity structures, in a degenerate optical parametric oscillator. We show that the mean-field and the propagation models predict the same increase in the domain size proportional to t(1/3) .

6.
Phys Rev A ; 53(2): 1072-1080, 1996 Feb.
Artigo em Inglês | MEDLINE | ID: mdl-9912986
9.
10.
Phys Rev A ; 41(12): 6635-6646, 1990 Jun 15.
Artigo em Inglês | MEDLINE | ID: mdl-9903077
13.
Phys Rev Lett ; 56(4): 274-277, 1986 Jan 27.
Artigo em Inglês | MEDLINE | ID: mdl-10033145
14.
Opt Lett ; 9(6): 243-5, 1984 Jun 01.
Artigo em Inglês | MEDLINE | ID: mdl-19721558

RESUMO

We report what to our knowledge are the first observations of an increase in the on-axis intensity of an intense cw on-resonance beam resulting from nonlinear absorption and diffraction during its propagation through a highly absorbing medium (sodium vapor). This "self-focusing" is not a self-lensing; instead it is modeled well by placing an aperture part way through the cell: The stripping by the aperture approximates the effect of the nonlinear absorption, and then Fresnel diffraction results in on-axis minima and maxima.

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