2020
DOI: 10.3389/fphy.2020.00096
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Non-linear Thermo-Optical Properties of MoS2 Nanoflakes by Means of the Z-Scan Technique

Abstract: The non-linear thermo-optical response of MoS 2 nanoflakes was investigated using the Z-scan technique, employing TM00-mode with a CW-laser diode operating at a wavelength of 532 nm. The systems were found to display a strong non-linear response, dominated by non-linear refraction. The effect of the thickness of the MoS 2 layer, deposited on a glass substrate, on the non-linear susceptibility was studied. Furthermore, in this study, the effects of modifying the thickness of the MoS 2 nanoflakes on the non-line… Show more

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Cited by 8 publications
(3 citation statements)
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“…Third‐order nonlinear susceptibility is calculated by using the following Equation () false| χ false( 3 false) false| = false[ false( R e false( χ false( 3 false) false) false) 2 + false( I m false( χ false( 3 false) false) false) 2 false] 1 / 2 where the light speed (c), the vacuum permittivity ( ε 0 ), the linear refractive index ( n 0 ), and the angular frequency ( ω ) of laser light, which is equal to 2 π c λ . All obtained open aperture fs z ‐scan results exhibit saturable absorption (SA) [ 44,45 ] as shown in Figure 10. Based on this theory, the obtained results for MoO 3 ultrathin films S0, S1, and S2 are shown in Table 4.…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…Third‐order nonlinear susceptibility is calculated by using the following Equation () false| χ false( 3 false) false| = false[ false( R e false( χ false( 3 false) false) false) 2 + false( I m false( χ false( 3 false) false) false) 2 false] 1 / 2 where the light speed (c), the vacuum permittivity ( ε 0 ), the linear refractive index ( n 0 ), and the angular frequency ( ω ) of laser light, which is equal to 2 π c λ . All obtained open aperture fs z ‐scan results exhibit saturable absorption (SA) [ 44,45 ] as shown in Figure 10. Based on this theory, the obtained results for MoO 3 ultrathin films S0, S1, and S2 are shown in Table 4.…”
Section: Resultsmentioning
confidence: 99%
“…where the light speed (c), the vacuum permittivity (ε 0 ), the linear refractive index (n 0 ), and the angular frequency (ω) of laser light, which is equal to 2πc λ . All obtained open aperture fs z-scan results exhibit saturable absorption (SA) [44,45] as shown in Figure 10. Based on this theory, the obtained results for MoO 3 ultrathin films S0, S1, and S2 are shown in Table 4.…”
Section: Nonlinear Photonic Behaviors Of Moo 3 Ultrathin Filmsmentioning
confidence: 90%
“… 10 Wang et al employed antimonene in Er- and Tm-doped fiber lasers to realize ultrafast lasers with mode-locked pulse output. 11 Recently, owing to copious applications in opto-electronics, there is a growing interest for low-dimensional materials with second and third order nonlinearities such as few-layer graphene, 12 2D graphdiyne, 13 MoS 2 nanoflakes, 14 semi-organic single-crystal, 15 metallic oxide thin film, 16,17 low-dimensional material from bismuth oxyhalide 18 and so on. Shinji Yamashita focused on the nonlinear optical properties of graphene and carbon nanotube to further their superior application value in fiber lasers, modulators, and other fields.…”
Section: Introductionmentioning
confidence: 99%