Nanoparticle Size and Concentration Estimation by - CNR-ISM
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Nanoparticle Size and Concentration Estimation by - CNR-ISM
Combined LAser Nanotechnology Nanoparticle Size and Concentration Estimation by Calibration Line Method by Laser-Induced Breakdown Spectroscopy Can Korala,*, Marcella Dell’Aglio b, Remah ElRashedy a, Rosalba Gaudiuso a,b, Alessandro De Giacomoa,b aDepartment of Chemistry, University of Bari “Aldo Moro”, Bari, 70126, Italy bCNR-IMIP sec. Bari, Bari, 70126, Italy *Can Koral, [email protected] It was observed that Ag I emission intensity during LIBS of Ag NPs deposited on Si is linearly correlated with concentrations and dimensions of colloids. • The LIBS signal of NPs appears to vary consistently with the change in concentration of the NPs, and to be affected as well by the particle size when the concentration of Ag atoms is kept constant. Ag NPs of different size produced by laser ablation in liquid [1]. • 14000 12000 10nm AgNPs 0.02 mg/ml in aqueous buffer, NanoComposix, Inc. Intensity (a.u.) 20nm AgNPs 0.02 mg/ml in buffer, Sigma Aldrich Co. 10000 aqueous 14000 20nm AgNPs (0.020 g/ml) 20nm AgNPs (0.010 g/ml) 10nm AgNPs (0.020 g/ml) 10nm AgNPs (0.010 g/ml) 10000 8000 6000 4000 2000 0 328.0 10nm AgNPs (0.020 g/ml) 10nm AgNPs (0.016 g/ml) 10nm AgNPs (0.010 g/ml) 10nm AgNPs (0.004 g/ml) 12000 Intensity (a.u.) • Having a fast technique for size and concentration characterization of NPs solutions is of extreme importance for the orientation of NPs to industrial and daily life products. • 8000 6000 4000 2000 328.5 329.0 339.0 339.5 0 328.5 340.0 329.0 Wavelength (nm) 339.0 339.5 340.0 Wavelength (nm) 8nm AgNPs by Ablation A series of solutions with different concentrations were prepared by direct dilution by deionised water Particle size distributions were characterized by UV-VIS spectrometer and absorption results were crosschecked with certified AgNPs dispersions • Highly reproducible calibration lines with a correlation factor close to unity were attained by using the standard calibration curve method [2]. • It has been found that slope is strictly dependent on the size of the NPs in the solution such that the average NPs size and their concentration have been determined with a limit of detection of few ppb. 20nm AgNPs 6000 5000 Intensity (a.u.) 4000 0.5µl drops of NPs colloids were put on silicon wafer substrate. y=2534x-101 R=0.96 3000 2000 1000 The solution was then evaporated by a focused single laser shot to form a homogeneous coating layer of NPs on a circular area of 3.5 mm in radius. 0 0.2 0.4 0.6 0.8 1.0 Relative Concentration • In this work a specifically designed Laser-Induced Breakdown Spectroscopy (LIBS) setup was constructed to characterize the NPs size and the concentration of the colloids. The acquisition conditions were: Time Delay 800 ns, Gate Width 10 µs, Laser Fluence 5 J/cm2, Spot Size 3.5mm. 10nm AgNPs 6000 5000 4000 Intensity (a.u.) • The LIBS Setup: Q-switched Nd:YAG laser (Quanta System, model: Giant 770-10) 3000 2000 1000 0 Monochromator 250nm/750 nm range, 1800 grooves/mm grating (Jobin Yvon Horiba TRIAX 550) 0.2 0.4 0.6 0.8 1.0 Relative Concentration 8nm AgNPs The laser pulse @ 1064nm was focused on to the target by a lens of (f:100 mm), the emitted light was reflected by an aluminum mirror(Ø:50 mm), the reflected beam was collected through a biconvex UV fused silica lens(f:75 mm) directly on to the monochromator entrance slit. The target was rotated such that the laser spot coincides with the rotation axis and to ensure the laser spot to cover all the area contaminated by the NPs 6000 5000 y=5789-547 R=0.91 4000 Intensity (a.u.) Intensified Charge Coupled Device (ICCD) (Jobin Yvon Horiba CCD-3000). A digital delay/pulse generator (Stanford Research Systems model: DG535) y=5311x-866 R=0.98 3000 2000 1000 AgNPs produced by Laser Ablation 0 • Each emission spectrum was acquired in multi shot mode by averaging the acquired spectra taken from the rotating target. 0.2 0.4 0.6 Relative Concentration References: [1] A. De Giacomo , M. Dell'Aglio , A. Santagata , R. Gaudiuso , O. De Pascale , P. Wagener , G. C. Messina , G. Compagnini andS. Barcikowski Phys. Chem. Chem. Phys.,15, (2013),3083-3092 [2] R. Gaudiuso, M. Dell'Aglio, O. De Pascale, G.S. Senesi, A. De Giacomo, Sensors 10 (2010) 7434-7468. Acknowledgements This poster draws on work undertaken as part of the project CLaN (Combined Laser Nanotechnology) co-financed by the Operational Programme ERDF Basilicata 2007-2013. 0.8 1.0