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It is also noteworthy to point out the differences in organic component admixtures observed when using the different laser excitations on the same analyses spot.
Figure 2a shows absorbance spectra of the colloidal suspensions prepared using the different laser pulse energies, and Fig. 2b presents the dependence of the basic features of the absorption plasmon band (APB) namely its center wavelength (CWL), full width at half maximum (FWHM), and maximum intensity on the laser pulse energy.
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Mann-Whitney U and Kruskal-Wallis H tests were used to compare the different laser output powers.
The pictures were acquired using frame λ, meaning that the different laser channels were collected one by one instead as simultaneously.
The sites were captured using two different laser scanning systems, the Leica C10 and the Trimble TX5.
Note that even though the earlier study was performed using a different laser excitation frequency (647 nm), almost all of the bands appear at similar frequencies and intensities as in the resonance Raman spectrum shown in Figure 2 recorded using 785 nm excitation.
Samples were measured in both the radial breathing mode and tangential mode ranges using three different laser lines.
The experiments were carried over a wide range of intensities using two different laser amplifier systems.
Raman spectra are recorded using two different laser power densities of 0.2 and 0.88 kW/cm2 for both the samples.
Laser-induced fluorescence measurements were carried out on two separate occasions using two different laser setups to study CO and CO2, respectively, but the catalysis reactor, MS setup, crystal sample, and associated experimental conditions were the same in both cases (see Figure 1).
c and d are typical Raman spectra (type A,B) from isolated individual SWNTs using two different laser excitations 2.41 and 1.96 eV.
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