2015
DOI: 10.1088/0957-4484/26/45/455303
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Pattern formation on silicon by laser-initiated liquid-assisted colloidal lithography

Abstract: We report sub-diffraction limited patterning of Si substrate surfaces by laser-initiated liquid-assisted colloidal lithography. The technique involves exposing a two-dimensional lattice of transparent colloidal particles spin coated on the substrate of interest (here Si) immersed in a liquid (e.g. methanol, acetone, carbon tetrachloride, toluene) to a single picosecond pulse of ultraviolet laser radiation. Surface patterns formed using colloidal particles with different radii in the range 195 nm ≤ R ≤ 1.5 μm a… Show more

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Cited by 6 publications
(10 citation statements)
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References 24 publications
(41 reference statements)
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“…by tuning n with the LILAC lithography method) rather than simply irradiating in air, but is not able to predict diffraction effects due to the presence of the sphere boundary. The |E 2 | vs X profiles clearly illustrate how the colloidal particle acts as a convergent (n > 0) or divergent (n < 0) lens [6], and how immersing the particle in different liquid media provides a route to extending the focal length of the NF-F region [11]. Compared with NF-LA in air, where ablation is localised to the region of contact between the particle and the substrate (i.e.…”
Section: Resultsmentioning
confidence: 99%
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“…by tuning n with the LILAC lithography method) rather than simply irradiating in air, but is not able to predict diffraction effects due to the presence of the sphere boundary. The |E 2 | vs X profiles clearly illustrate how the colloidal particle acts as a convergent (n > 0) or divergent (n < 0) lens [6], and how immersing the particle in different liquid media provides a route to extending the focal length of the NF-F region [11]. Compared with NF-LA in air, where ablation is localised to the region of contact between the particle and the substrate (i.e.…”
Section: Resultsmentioning
confidence: 99%
“…Thus n < 0 in these examples and the NF-F patterns will appear as an ablation ring rather than the localized ablation crater seen in the case of NF-LA in air. The radius of this ablation ring (relative to the centre of the colloidal particle) can be tuned by changing the size of the colloidal particle or the magnitude of n [6]. The NF-S rings are again confined to areas outside the radius of the colloidal particle but, as we show below, the topographies can be very different from those formed in air.…”
Section: Surface Patterning Under a Liquidmentioning
confidence: 87%
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“…Albeit a slowdown in process speed, a straightforward method to overcome diffraction limit was seen in processing using optical evanescent fields from the tip of an optical fiber [12] or microscope probes [13,14] in a scanning near-field microscopy approach. The possibility to work in the near-field was extrapolated to the use of microspheres self-organized on surfaces [15,16], a way to equally parallelize the interaction.…”
Section: Introductionmentioning
confidence: 99%
“…Our recently demonstrated Laser Induced Liquid Assisted Colloidal (LILAC) lithography technique [ 14 , 15 ] allows complex patterning of substrates using single laser pulses and isolated, or small arrays of, colloidal particles immersed in a liquid. Two distinct contributions to the patterning were identified: (a) near-field laser ablation (NF-LA) rings, caused by near-field intensity enhancement effects, and (b) near field scattering (NF-S) ring structures with characteristic minima and maxima that arise as a result of interference between the incident laser beam, light reflected at the substrate surface, and light scattered by the particle.…”
Section: Introductionmentioning
confidence: 99%