The concept of guiding light with light and negative third-order optical nonlinearities of organics

Dark spatial solitons can be used for generating light-induced waveguides and guiding light with light. A negative (self-defocusing) third-order nonlinearity is necessary to generate dark solitons. We show that the negative electronic nonlinearity is possible at 800 nm in several classes of organics including squaraine dyes, -conjugated polymers of poly(p-phenylenevinylene) type and polyaniline.

[1]  F Noack,et al.  Frequency upconversion of tunable femtosecond pulses by parametric amplification and sum-frequency generation in a single nonlinear crystal. , 1995, Optics letters.

[2]  A. Samoc,et al.  Real and imaginary components of the third-order nonlinearity of polyaniline dodecylbenzenesulfonic salt. , 1995, Optics letters.

[3]  A. Snyder,et al.  Stable black self-guided beams of circular symmetry in a bulk Kerr medium. , 1992, Optics letters.

[4]  B Luther-Davies,et al.  Tuning the properties of poly(p-phenylenevinylene) for use in all-optical switching. , 1995, Optics letters.

[5]  Jean-Michel Nunzi,et al.  Phase and frequency resolution of picosecond optical Kerr nonlinearities. , 1991, Optics letters.

[6]  D. R. Andersen,et al.  Observation of fundamental dark spatial solitons in semiconductors using picosecond pulses. , 1991, Optics letters.

[7]  B Luther-Davies,et al.  Steerable optical waveguides formed in self-defocusing media by using dark spatial solitons. , 1992, Optics letters.

[8]  A. Snyder,et al.  Spatial solitons of the power-law nonlinearity. , 1993, Optics letters.

[9]  P. Prasad,et al.  Dynamics of third‐order nonlinearity of canthaxanthin carotenoid by the optically heterodyned phase‐tuned femtosecond optical Kerr gate , 1993 .

[10]  Donal D. C. Bradley,et al.  Precursor route chemistry and electronic properties of poly(p-phenylenevinylene), poly[(2,5-dimethyl-p-phenylene)vinylene] and poly[(2,5-dimethoxy-p-phenylene)vinylene] , 1992 .

[11]  C. Froehly,et al.  Spatial-soliton-induced guided waves in a homogeneous nonlinear Kerr medium. , 1991, Optics letters.

[12]  Paras N. Prasad,et al.  Optical heterodyning of the phase‐tuned femtosecond optical Kerr gate signal for the determination of complex third‐order susceptibilities , 1992 .

[13]  Mark G. Kuzyk,et al.  Mechanisms of quadratic electro-optic modulation of dye-doped polymer systems , 1990 .

[14]  H. Engan,et al.  All-fiber acousto-optic frequency shifter excited by focused surface acoustic waves. , 1991, Optics letters.

[15]  W. Ziegenbein,et al.  The Cyclobutenediylium Cation, a Novel Chromophore from Squaric Acid , 1967 .

[16]  Mark G. Kuzyk,et al.  A simplified three‐level model describing the molecular third‐order nonlinear optical susceptibility , 1992 .

[17]  Barry Luther-Davies,et al.  Photophysical Processes Involved in Creation of Dark Spatial Solitons in Composite Photonic Media , 1994 .

[18]  A. Snyder,et al.  Self-induced optical fibers: spatial solitary waves. , 1991, Optics letters.

[19]  Jean-Michel Nunzi,et al.  Femtosecond Kerr ellipsometry in polydiacetylene solutions: Two-photon effects , 1993 .

[20]  Regan,et al.  Spatial dark-soliton stripes and grids in self-defocusing materials. , 1991, Physical review letters.

[21]  A. Schmidt Reaktionen von Quadratsäure und Quadratsäure-Derivaten , 1980 .

[22]  Nonlinear-optical properties of a poly(vinyl alcohol)-polyaniline interpenetrating polymer network. , 1995, Optics letters.

[23]  E. W. Stryland,et al.  Sensitive Measurement of Optical Nonlinearities Using a Single Beam Special 30th Anniversary Feature , 1990 .