2013
DOI: 10.1364/oe.21.001986
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Pulsed laser manipulation of an optically trapped bead: Averaging thermal noise and measuring the pulsed force amplitude

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Cited by 8 publications
(7 citation statements)
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“…Inspired by this deduction, researchers have utilized pulsed lasers to eject particles initially attached on a glass substrate, which could then be captured and levitated by a conventional CW light optical tweezer after detachment [241,242] . In corresponding works, the axial gradient force of the pulsed laser would “kick” the attached particle in a pulsed fashion, and the detachment would not occur until the transient kick surmounts the strength of van der Waals force, which is estimated to be at nanonewton level in experimental scenarios (the situation here differs from those where actuators locomote “along” the substrate surface and experience stronger adhesive forces at μN scale) [242,243] . Considering the transparency of both the particles and substrate to incident light and also the fact that such a large force is beyond reach of a CW light optical tweezer with mW power output, the axial optical force (which also includes the scattering force) of the pulsed laser, the peak power of which is at W scale, becomes the sole reason for particle ejection.…”
Section: Optical Manipulation In Solid Environmentsmentioning
confidence: 99%
“…Inspired by this deduction, researchers have utilized pulsed lasers to eject particles initially attached on a glass substrate, which could then be captured and levitated by a conventional CW light optical tweezer after detachment [241,242] . In corresponding works, the axial gradient force of the pulsed laser would “kick” the attached particle in a pulsed fashion, and the detachment would not occur until the transient kick surmounts the strength of van der Waals force, which is estimated to be at nanonewton level in experimental scenarios (the situation here differs from those where actuators locomote “along” the substrate surface and experience stronger adhesive forces at μN scale) [242,243] . Considering the transparency of both the particles and substrate to incident light and also the fact that such a large force is beyond reach of a CW light optical tweezer with mW power output, the axial optical force (which also includes the scattering force) of the pulsed laser, the peak power of which is at W scale, becomes the sole reason for particle ejection.…”
Section: Optical Manipulation In Solid Environmentsmentioning
confidence: 99%
“…When targeting the modulation and delivery modules, correctly under filling microscope objectives with laser illumination can be used to optimize the available power [60]. Reaching the nanonewton (nN) optical force domain can either be done in the particle module using antireflection-coated beads [61], or in the source module by just using regular beads but replacing the light source with a short-pulsed laser [62]. Moreover, by moving beyond the standard microspheres, microfabrication-tailored particle shapes can be used to create optically steered microtools [63], which we will discuss further in Section 4.…”
Section: Experimental Geometries and Strategiesmentioning
confidence: 99%
“…Hence, similar to the argumentation given in Ref. 19, we derived an expression for the expectation value of the power spectral density (see supplementary material 25 )…”
mentioning
confidence: 92%
“…The switching process (on/off) is controlled by blocking the laser output in intervals with a chopper wheel. By applying a post-elimination technique 19,20 for thermal noise based on a lock-in strategy, a force sensitivity of 2.4 fN is obtained. This value is lower than the force sensitivity obtained before in the context of optical tweezers applications in liquids.…”
mentioning
confidence: 99%
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