NOEL

Semiconductor processes and nanofabrication


 

High-efficiency photo-electron conversion devices

Semiconductor processes and nanofabrication

Characterizations and applications of nanomaterials

Light harvesting and light extraction

Optical analysis techniques

Eco-friendly devices and sensors

 

 


 

 


 

Laser-induced jets of nanoparticles: exploiting air drag forces to select the particle size of nanoparticle arrays

In this study, we developed a new method—based on laser-induced jets of nanoparticles (NPs) and air drag forces—to select the particle size of NP arrays. First, the incident wavelength of an excimer laser was varied to ensure good photo-to-thermal energy conversion efficiency. We then exploited air drag forces to select NPs with sizes ranging from 5 to 50 nm at different captured distances. Controlling the jet distances allowed us to finely tune the localized surface plasmon resonance (LSPR) wavelength. The shifting range of the LSPR wavelengths of the corresponding NP arrays prepared using the laser-induced jet was wider than that of a single NP or an NP dimer. We further calculated the relationship between the air drag force and the diameter of the NPs to provide good control over the mean NP size (capture size S 300 mm) by varying the capture distance. Laser-induced jets of NPs could also be used to fabricate NP arrays on a variety of substrates, including Si, glass, plastic, and paper. This method has the attractive features of rapid, large-area preparation in an ambient environment, no need for further thermal annealing treatment, ready control over mean particle size, and high selectivity in the positioning of NP arrays. Finally, we used this method to prepare large NP arrays for acting hot spots on surface-enhanced Raman scattering-active substrates, and 1012 M R6G can be detected. Besides, we also prepare small NP arrays to act as metal catalysts for constructing low-reflection, broadband light trapping nanostructures on Si substrates.


a) Schematic representation of a laser-induced jet of NPs. (b) Reflectance and (c) absorbance spectra of metal films having a thickness of 35 nm. (d) Transmittance, reflectance, and absorbance spectra of Au films of various thicknesses at wavelength of 248 nm.

(a) Absorption spectra of NPs captured at different distances between the source and receiving plates. (b) Extinction spectra of single NPs of various sizes, simulated using the 3D-FDTD method. (c) Extinction spectra of NP arrays of dimers of NPs of various sizes, simulated using the 3D-FDTD method. (d) Comparison of simulated and measured extinction wavelengths of NPs.

 

 



 
 
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