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Determination of the third- and fifth-order optical nonlinearities: the general case

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Abstract

We compute the evolution of the intensity (I) and the phase (φ) of a beam propagating in a nonlinear (NL) isotropic medium exhibiting third- and fifth-order NL optical characteristics. All formulas are analytic, but the general case requires a numerical inversion by means of Newton’s method. The solutions may differ if some coefficients vanish, so they are given in all cases up to the fifth-order nonlinearities. The analytical relations allow us to fit the experimental data using the recently introduced D4σ-Z-scan method. Carbon disulfide is tested at 532 and 1,064 nm in the picosecond regime deducing NL coefficients related to third- and fifth-order optical susceptibilities.

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Correspondence to V. Besse.

Appendices

Appendix 1: Solution for z(I)

See Table 1.

Appendix 2: Solution for the nonlinear phase shift Δφ(I)

See Table 2.

Appendix 3: Summary of the measured nonlinear coefficients

See Table 3.

Table 3 Summary of the third- and the fifth-order measured nonlinear coefficient values for CS2 in the picosecond regime with linearly polarized light

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Besse, V., Boudebs, G. & Leblond, H. Determination of the third- and fifth-order optical nonlinearities: the general case. Appl. Phys. B 116, 911–917 (2014). https://doi.org/10.1007/s00340-014-5777-2

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  • DOI: https://doi.org/10.1007/s00340-014-5777-2

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