Saturable absorption and nonlinear refraction in free-standing carbon nanotube film: Theory and experiment

• Published in: Carbon (New York) Vol. 186; pp. 509 - 519
• Main Authors: Vanyukov, V.V., Shuba, M.V., Nasibulin, A.G., Svirko, Y.P., Kuzhir, P.P., Mikheev, G.M.
• Format: Journal Article
• Language: English
• Published: New York Elsevier Ltd 01-01-2022; Elsevier BV
• Subjects: Absorption spectra; Absorptivity; Carbon; Dynamic Burstein–Moss shift; Femtosecond pulses; Free-standing carbon nanotube film; Kinetic equations; Nanotubes; Nonlinear refraction; Pulse duration; Refraction; Refractivity; Saturable absorption; Saturation; Single wall carbon nanotubes; Surface conductivity; Thin films; Free-standing carbon nanotube film; Saturable absorption; Dynamic Burstein–Moss shift; Nonlinear refraction; Surface conductivity
• ISSN: 0008-6223; 1873-3891
• DOI: 10.1016/j.carbon.2021.10.054

The nonlinear absorption and refraction of free-standing films made of single-walled carbon nanotubes (SWNTs) have been investigated experimentally and theoretically. By solving the quantum kinetic equations that take into account both the intra- and interband transitions, we obtain the analytical expression for the SWNT nonlinear conductivity. The nonlinear absorption coefficient and saturation intensity of the film comprising randomly orientated SWNTs have been calculated in a broad spectral range spanning over M11, S11, and S22 absorption bands. The effects of the laser pulse duration and dynamic Burstein−Moss shift on the saturation intensity have been revealed. We demonstrate in the experiment that, under irradiation with femtosecond laser pulses, the absorption modulation depth of SWNT film at resonance wavelength 1375 nm is as high as 30%. The observed saturation intensity minimum is red-shifted with respect to the absorption maximum due to the dynamic Burstein−Moss shift. The saturation intensity within the S22 band is 26−fold lower than that out of the band at 795 nm. The closed-aperture z-scan measurements reveal the negative nonlinear refractive index n2 = −3.1 × 10−12 cm2/W at 795 nm.
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