2019
DOI: 10.1364/ol.44.005214
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Nonlinear optical response spatial self-phase modulation in MoTe2: correlations between χ(3) and mobility or effective mass

Abstract: We report an unambiguous observation of third-order nonlinear optical effect, spatial self-phase modulation (SSPM), in a MoTe 2 dispersion. The values of the third order nonlinear optical coefficients effectively for one layer MoTe 2 , χ (3) one-layer , are obtained through the SSPM method at excitation wavelengths 473, 532, 750 and 801 nm, respectively. The wind-chime model is used to explain the ring formation time. The wavelength dependence of χ (3) one-layer compares well with the photo-absorption spectra.… Show more

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Cited by 35 publications
(42 citation statements)
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“…Thus far, SSPM has become a typical effective means to characterize 2D materials' nonlinear optical response. The n 2 (nonlinear refractive index) and v 3 ð Þ (third-order nonlinear susceptibility) of numerous materials, including graphene [14], tellurium [15], mote 2 [16], antimonene [17], etc., have been obtained by this method.…”
Section: Introductionmentioning
confidence: 99%
“…Thus far, SSPM has become a typical effective means to characterize 2D materials' nonlinear optical response. The n 2 (nonlinear refractive index) and v 3 ð Þ (third-order nonlinear susceptibility) of numerous materials, including graphene [14], tellurium [15], mote 2 [16], antimonene [17], etc., have been obtained by this method.…”
Section: Introductionmentioning
confidence: 99%
“…The time evolution of the diffraction ring number ( N ) can be fitted by an exponential decay model, N=Aet/τnormalrise, where τ rise is the rise time for ring formations, and A denotes a constant. [ 44 ] According to the wind chime model proposed by Zhao et al., the formation time of the diffraction ring is described as T=εrπηξRc1.72(εr1)Ih, where ε r is the relative dielectric constant of the 2D material, η is the viscosity coefficient of the solvent, ξ is the fluid property of the 2D material, R is the average radius of the nanosheet disk, and I is the laser intensity. [ 24 ] The SSPM effect of most materials is almost instantaneous; however, this is not the case in some photopolymers (e.g., organ siloxanes).…”
Section: Fundamentals Of 2d Material‐based Sspmmentioning
confidence: 99%
“…achieved nonlinear tuning of the broadband nonlinear refractive index in the time dimension, with the maximum Δn2/n2 approaching 90% (Figure 2i). [ 162 ] Although the formation time of the SSPM effect can be changed, [ 44 ] the nonlinear tuning in the time dimension remains difficult to control. The same effect can be achieved at the temperature scale, which may be caused by thermally induced nonlinearity or bubble scattering (Figure 2j).…”
Section: State Of the Art Of 2d Material‐based Sspmmentioning
confidence: 99%
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