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b The 150th row cross-section intensity of Fig. 5a c.

The 150th row cross-section intensity of Fig. 5a c is shown in Fig. 6b.

Cross-section intensity at the red line position showing in a c is analyzed in Fig. 6b.

The extinction cross-section intensity of the longitudinal mode is strongly polarisation dependent.

The cross-section intensity for each emulsion was normalized to the mean intensity along the emulsion boundary.

The peak intensity ratio was determined to be 4.3, serving as an indicator for synthesis quality, as spherical impurities will add up to the T-LSPR cross-section intensity.

The intensity cross section of the fluorescence intensity obtained for these three nanoparticles is shown in Figure 2c.

Herein, a novel nanostructure material was designed by S1 (2, 2': 6′, 2″-terpyridyl derivative Zn SCN 2 complex) modified gold nanoparticles with obvious improving two photon absorption (TPA) cross section, the fluorescence intensity, lifetime, fluorescence quantum yield due to the enhancement of intramolecular charge transfer (ICT) process.

This GaAs layer is pumped by 1319 nm higher order Gaussian beam of a Nd YAG laser, which passes through a cylindrical lens thereby generating a high aspect ratio elliptical cross section to attain intensity dependent negative extinction coefficient on that 3 mm long strip of irradiated GaAs.

An intensity cross section displayed in Figure 3c features the increase of the intensity at the edges of the nanoparticles; however, the scale of the enhancement is lower than that in the case of 1,100-nm 1,100-nms.

(c) Cross section of the fluorescence intensity obtained for the three nanoparticles shown in Figure 2a.