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Fifth-order optical nonlinearity of pseudoisocyanine solution at 529 nm

R. A. GaneevInstitute for Solid State Physics, University of Tokyo, 5-1-5 Kashiwanoha, Kashiwa,#N#Chiba 277-8581,#N#JapanM. BabaInstitute for Solid State Physics, University of Tokyo, 5‐1‐5 Kashiwanoha Kashiwa, Chiba 277‐8581, JapanMakoto MoritaDepartment of Applied Chemistry, Faculty of Engineering, Seikei University, Kichijoji, Musashino-shi, Tokyo 180-8633, JapanA.I. RyasnyanskySamarkand State University, Samarkand 703004,#N#UzbekistanM. SuzukiInstitute for Solid State Physics, University of Tokyo, 5‐1‐5 Kashiwanoha Kashiwa, Chiba 277‐8581, JapanM. TuruInstitute for Solid State Physics, University of Tokyo, 5‐1‐5 Kashiwanoha Kashiwa, Chiba 277‐8581, JapanHiroto KurodaInstitute for Solid State Physics, University of Tokyo, 5‐1‐5 Kashiwanoha Kashiwa, Chiba 277‐8581, Japan
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Evidence of the interference between third- and fifth-order nonlinear optical processes is shown in the studies of pseudoisocyanine (PIC) dye aqueous solution using 529 nm radiation (t = 475 fs) and the Z -scan technique. The third-order nonlinear refractive index of the PIC solution was measured to be −8 × 10 −14 cm 2 W −1 .W e have shown th at PIC solution changes from being self-defocusing to self-focusing at high laser intensity that was attributed to the influence of fifth-order nonlinearity. The fifth-order nonlinear refractive index was measured to be 4 × 10 −24 cm 4 W −2 .T he bleaching properties of PIC solution were analysed, and the imaginary part of third-order nonlinear susceptibility was measured to be Im χ (3) =− 2 × 10 −12 esu.

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