15 research outputs found

    Response of HEK cells to dielectrophoresis for increasing medium conductivities.

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    <p>nDEP and pDEP are applied at <i>f</i>  =  1 kHz and <i>f</i>  =  200 kHz, respectively. The arrow represents cell motion during 5 frames (300 ms), the picture being the last image. DEP is stronger at low conductivities compared to EHD forces so cells experience larger displacement at higher velocities at low conductivities.</p

    Rotation study of three human cell lines.

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    <p><b>(a1)</b> Time-lapse sequence images of the rotation of HEK cells in the z-axis, in presence of 1 µm polystyrene colloid (highlighted in blue circles). Particles were added to observe medium stream lines. The red circle pinpoints a visible organelle. Rotation is studied at σ<sub>m</sub>  =  2.10<sup>−2</sup> S/m when varying <b>(a2)</b> magnitude of the electric field at <i>f</i>  =  45 kHz or <b>(a3)</b> frequency at magnitude 0.065 V/µm (V = 10 Vp-p). The dashed line plots the values of |Re[CMF(ω)]| at the same frequencies, bringing out the relation between DEP effect and ETE. Rotation studies of <b>(b)</b> of JURKAT cells and <b>(c)</b> PC3 cells (electric field magnitude is 0.089 V/µm (V = 4Vp-p) and σ<sub>m</sub>  =  2 10<sup>−2</sup> S/m.). The inset on the lower part of the graphs shows the number of cells used for each mean value.</p

    Table of the dielectric parameters for three human cell lines.

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    <p>The cytoplasm conductivity σ<sub>3</sub> and membrane capacitance <i>C<sub>mem</sub></i> are calculated from experimental fit to the competitive model.</p

    Summary of cells behaviors at (a) σ<sub>m</sub>  =  2.10<sup>−4</sup> S/m and (b) σ<sub>m</sub>  =  2.10<sup>−2</sup> S/m.

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    <p>Photographs and schemes illustrate the cell motion for typical frequencies and magnitudes with corresponding graphs of the DEP (U<sub>DEP</sub>, green line) and EHD (U<sub>EHD</sub>, in red) velocities. The velocities were calculated according to the theoretical model presented in the first paragraph and position of the field was taken for x = 1 µm. The boxed text refers to the related paragraph.</p

    A near-field actuated optical nanocavity

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    International audienceWe demonstrate here that switching and tuning of a nanocavity resonance can be achieved by approaching a sub-micrometer tip inside its evanescent near-field. The resonance energy is tuned over a wide spectral range (/~10-3) without significant deterioration of the cavity peaktransmittance and of the resonance linewidth. Such a result is achieved by taking benefits from a weak tip-cavity interaction regime in which the tip behaves as a pure optical path length modulato

    On-chip photonic tweezers for photonics, microfluidics, and biology

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    International audienceNear-field optical forces arise from evanescent electromagnetic fields and can be advantageously used for on-chip optical trapping. In this work, we investigate how evanescent fields at the surface of photonic cavities can efficiently trap micro-objects such as polystyrene particles and bacteria. We study first the influence of trapped particle’s size on the trapping potential and introduce an original optofluidic near-field optical microscopy technique. Then we analyze the rotational motion of trapped clusters of microparticles and investigate their possible use as microfluidic micro-tools such as integrated micro-flow vane. Eventually, we demonstrate efficient on-chip optical trapping of various kinds of bacteria
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