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Optical cubic nonlinearity of thin two-layer AuNP–Al2O3 and three-layer AuNP–Al2O3–PdO systems under nanosecond 1064 nm and 532 nm excitation

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Abstract

Triple-layered structures, containing gold nanoparticles (AuNP), namely AuNP(6 nm)–Al2O3(1.5 nm)–PdO(17 nm), sample #1, and AuNP(6 nm)–Al2O3(13 nm)–PdO(17 nm), sample #2, were obtained on glass substrates. A significant difference in the structure of their absorption spectra in the vicinity of the plasmon resonance of gold nanoparticles indicates a dependence on the mutual influence of the AuNP and PdO layers on the thickness of the Al2O3 insulating layer. Optical cubic nonlinearity (OCN) parameters, namely n2, Reχ(3), and Imχ(3), were determined for nanosecond pulsed laser excitation at λ = 1064 nm (τp = 15 ns) and λ = 532 nm (τp = 9 ns). It is shown that under 1064 nm excitation: (i) the sign of the refractive nonlinearity of the structures depends on the way they are illuminated in a Z-scan experiment, being positive when the laser beam impinges from the AuNP side (geometry A) and negative if the beam falls from the PdO side (geometry B); (ii) the nonlinear index of refraction n2 = 2.5 × 10–7 cm2/W of the structure #1 with a 1.5 nm thick Al2O3 layer is significantly larger than n2 = 0.9 × 10–7 cm2/W of the structure #2 with a 13 nm Al2O3 layer; (iii) the refractive nonlinearity of triple-layer structures is larger than that of double-layer structures AuNP-Al2O3; (iv) both double and triple-layer structures demonstrate moderate non linear absorption (β ~ 10–2 cm/W), probably due to two-photon transitions between the d and sp bands of AuNP. For 532 nm excitation, the refractive nonlinearity of the triple layer structures is negative with |n2|~ 10–6 cm2/W irrespective of the geometry of the Z-scan experiment. For both samples #1 and #2 with different thickness of Al2O3 the value of |n2| is sufficiently larger than one for separate PdO film. This may be explained by the strong influence of interaction of processes in the AuNP and conductive PdO layers. The nonlinear absorption coefficient β is negative (saturable absorption) in AuNP-Al2O3 structures and positive in AuNP-Al2O3-PdO structures.

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The datasets generated during and/or analyzed during the current study are available from the corresponding author upon reasonable request.

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Funding

This work was performed within project B-189 of the target complex program of basic research of the NAS of Ukraine.

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V.I. Rudenko, M.S. Brodyn, and A.M. Brodin wrote the main manuscript text. V.I. Rudenko performed experiments to determine spectra and measure nonlinear characteristics. V.I. Styopkin prepared the samples and participated in the discussion of the results of the experiments. V.R. Liakhovetskyi prepared figures and participated in the discussion of the results of the experiments. All authors reviewed the manuscript.

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Correspondence to Valentyn Rudenko.

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Rudenko, V., Brodyn, M., Liakhovetskyi, V. et al. Optical cubic nonlinearity of thin two-layer AuNP–Al2O3 and three-layer AuNP–Al2O3–PdO systems under nanosecond 1064 nm and 532 nm excitation. Opt Quant Electron 55, 420 (2023). https://doi.org/10.1007/s11082-023-04698-9

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  • DOI: https://doi.org/10.1007/s11082-023-04698-9

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