2010
DOI: 10.1364/oe.18.018483
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Flow-assisted Single-beam Optothermal Manipulation of Microparticles

Abstract: An optothermal tweezer was developed with a single-beam laser at 1550 nm for manipulation of colloidal microparticles. Strong absorption in water can thermally induce a localized flow, which exerts a Stokes' drag on the particles that complements the gradient force. Long-range capturing of 6 microm polystyrene particles over approximately 176 microm was observed with a tweezing power of approximately 7 mW. Transportation and levitation, targeted deposition and selective levitation of particles were explored to… Show more

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Cited by 27 publications
(22 citation statements)
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“…A careful choice of experimental conditionswith thermophoresis and liquid convection acting in opposite directions -can eventually lead to particle aggregation at locations where the two driving forces balance each other. This effect was used to realize optothermal traps for concentrating nanoparticles, such as DNA molecules [446][447][448], as well as microscopic colloids [449][450][451][452][453]. Such trapping mechanisms, however, do not allow for the selective targeting of individual particles and, thus, they are limited to manipulating large ensembles of molecules or colloids.…”
Section: Optically Induced Thermophoresismentioning
confidence: 99%
“…A careful choice of experimental conditionswith thermophoresis and liquid convection acting in opposite directions -can eventually lead to particle aggregation at locations where the two driving forces balance each other. This effect was used to realize optothermal traps for concentrating nanoparticles, such as DNA molecules [446][447][448], as well as microscopic colloids [449][450][451][452][453]. Such trapping mechanisms, however, do not allow for the selective targeting of individual particles and, thus, they are limited to manipulating large ensembles of molecules or colloids.…”
Section: Optically Induced Thermophoresismentioning
confidence: 99%
“…This morphology changes and redistribution of NRs are obviously due to the localized heating generated from NRs at the focal point. (2) However, there is no signal detected at the focal point and ring structure was observed, which can be explained by a repulsive optothermal flow and direct laser generated pushing flow at the focal point (Gu et al, ; Liu et al, ). This phenomenon also exists in Figure C, although it is not very obvious due to the free diffusion of NRs after trapping.…”
Section: Resultsmentioning
confidence: 99%
“…Even in a microfluidic channel with a typical dimension of 100–200 μm, the absorbed power at 1.5–1.6 μm in the microfluidic channel can be high enough to generate local heating (e.g. >10°C for a power of >10 mW)34, that can in turn influence the variability of optofluidic bioassays35 and also creates local fluidic flow for microparticle manipulation (based on photothermal tweezer)36. In contrast, such photothermal effect can be neglected at 1 μm.…”
Section: Discussionmentioning
confidence: 99%