We show, for the first time to our knowledge, that the fundamental beam that participates in the process of third-harmonic generation experiences an additional high-order nonlinear phase shift. The magnitude of the shift is proportional to the square of the pump intensity and the length of the sample and depends on the deviation from the exact phase-matched condition. This phase shift arises from cascaded third-order processes. Its value can exceed the value of the phase shift that originates from inherent fifth-order susceptibility of the nonlinear medium. Its sign is controllable by the sign of the phase mismatch of the third-harmonic generation process
The nonlinear phase shift associated with chi((2)) cascading was studied for ultrashort pulses in re...
Nonlinear phase shifts which increase with input irradiance can be generated in quadratically nonlin...
It is shown, both theoretically and experimentally, that during laser pulse filamentation in air an ...
In centrosymmetric media, in addition to the third- and fifth-order nonlinearity, a cascaded [Formul...
We show that processes such as second-harmonic generation and subsequent downconversion, and paramet...
We show that processes such as second-harmonic generation and subsequent downconversion, and paramet...
Beams that experience third-harmonic generation (THG) also experience Kerr effects. With Kerr effect...
Nonlinear phase shifts which increase with input irradiance can be generated in quadratically nonlin...
We propose a novel type of cascading parametric interaction for generating a nonlinear phase shift i...
Collinear third-harmonic generation at 526.7 nm was realized by the simultaneous phase matching of t...
Although the χ(2)(ω;2ω, -ω):χ(2)(2ω;ω,ω) cascading process utilizes the second-order susceptibility,...
An investigation of cascaded second-order optical effects resulting in effective third-order interac...
We compute the evolution of the intensity (I) and the phase (phi) of a beam propagating in a nonline...
The cascaded second-order nonlinearity arising from the second-harmonic generation process in noncen...
This paper concerns the theoretical, numerical, and experimental study of the second-harmonic-genera...
The nonlinear phase shift associated with chi((2)) cascading was studied for ultrashort pulses in re...
Nonlinear phase shifts which increase with input irradiance can be generated in quadratically nonlin...
It is shown, both theoretically and experimentally, that during laser pulse filamentation in air an ...
In centrosymmetric media, in addition to the third- and fifth-order nonlinearity, a cascaded [Formul...
We show that processes such as second-harmonic generation and subsequent downconversion, and paramet...
We show that processes such as second-harmonic generation and subsequent downconversion, and paramet...
Beams that experience third-harmonic generation (THG) also experience Kerr effects. With Kerr effect...
Nonlinear phase shifts which increase with input irradiance can be generated in quadratically nonlin...
We propose a novel type of cascading parametric interaction for generating a nonlinear phase shift i...
Collinear third-harmonic generation at 526.7 nm was realized by the simultaneous phase matching of t...
Although the χ(2)(ω;2ω, -ω):χ(2)(2ω;ω,ω) cascading process utilizes the second-order susceptibility,...
An investigation of cascaded second-order optical effects resulting in effective third-order interac...
We compute the evolution of the intensity (I) and the phase (phi) of a beam propagating in a nonline...
The cascaded second-order nonlinearity arising from the second-harmonic generation process in noncen...
This paper concerns the theoretical, numerical, and experimental study of the second-harmonic-genera...
The nonlinear phase shift associated with chi((2)) cascading was studied for ultrashort pulses in re...
Nonlinear phase shifts which increase with input irradiance can be generated in quadratically nonlin...
It is shown, both theoretically and experimentally, that during laser pulse filamentation in air an ...