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The total diode optical power is varied for both single and dual diode laser bar configurations.
The dual diode laser bar configuration, however, can be used to both stretch and optically trap cells at a fixed position.
The net cell deformation was found to be a function of the total laser power and not the power distribution between single or dual diode laser bar configurations.
Figure 4(a) and Fig. 4(b) illustrate the steady-state deformed shapes induced by both single and symmetric dual diode laser bar optical stretchers.
Here, the single diode laser bar and the symmetric dual diode laser bar deformation profiles are similar for the same total laser power.
Figure 2(a) and 2(b) provide a 2D side view and color map of the optical stress distribution on a 3D cell membrane in single and symmetric dual diode laser bar configurations at the same total laser power.
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Dual diodes with embedded silicon controlled rectifier (DD-SCR) for high-speed applications are presented.
Moreover, the dual-diode scheme provides a measure of self-correction, since both front and rear diode channels are subject to the same changes in temperature.
The dual-diode model at low-level radiation has fewer errors and is more accurate, and this makes the photovoltaic cells to have fewer errors and more accuracy in the shade.
The calculated spin transport characteristics reveal that such a chain-based device promises not only a perfect double spin-filtering effect, but also an excellent dual spin diode feature and a giant magnetoresistance (GMR) effect.
In this paper, we simulate the transient cell deformation induced by single and dual linear diode laser bar optical stretchers.
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