Liquid Drop Actuation by Photoelectrowetting

In electrowetting an electric potential is applied between a droplet of electrolyte and a conductor separated by an insulator. The repulsion of like charges deforms and spreads the droplet until capillary and electric forces are in equilibrium. Photoelectrowetting is a light-triggered version of electrowetting where the conductor is replaced by a moderately-doped semiconductor. The electrolyte-insulator-semiconductor stack resembles a metal-insulator-semiconductor capacitor, which has the special property that the amount of charge that can be injected into it increases when exposed to light. Thus in photoelectrowetting the exposure of light spreads the droplet further than in unilluminated conditions. In this thesis a scheme is presented for moving drops on a surface using photoelectrowetting. In order to understand photoelectrowetting I conducted a study of electrowetting with semiconductors. Devices were constructed using moderately-doped p-type silicon wafers (Na = 8.6 × 1014 cm−3) coated with a bilayer composed of thermal oxide (100 nm) and teflon (265 nm). Electric biases (< 40 V) were applied between droplets of electrolyte (10 microliter, 10 mM NaCl) and the silicon wafer, resulting in deformations of the droplet. These changes were quantified with contact angle measurements which varied from 120◦ at zero bias to 90◦ at 40V depending on the conditions of the experiment. Three regimes were observed depending on the polarity of the bias and above-bandgap illumination impinging on the droplet, corresponding to the charge regimes of an MIS capacitor: accumulation, inversion and deep-depletion. I present a model for these wetting changes based on a balance of capillary and electrostatic forces. After accounting for various non-ideal effects, I find that the model agrees with the data. I demonstrate that it is essential to account for interface traps in our devices (1.8 × 1011 cm−2) in the deep-depletion regime, leading to a 33% (4◦) correction to the prediction at 40V. I elucidate the nature of the photoelectrowetting effect and find that contrary to reports in the literature the transition is not reversible by light alone. In the next phase of my thesis, I demonstrate how photoelectrowetting triggered with a light beam on one side moves the droplet along a surface. Comparable with traditional electrowetting-based devices, I achieve speeds of up to 12 mm/s with 10 microliter drops of electrolyte (1% w/w NaCl) with a surfactant (5 mM NaCl) using an oscillating electric potential composed of an AC bias of magnitude 32.5 Vpp and a DC offset of −7 V cycled at a frequency of 15 kHz and a laser intensity of 40 mW/cm^2 (λ = 660nm). I measure the speed for varying magnitude and frequency of the bias, laser intensity, droplet size and viscosity. The optimal cycling frequency is set by competing effects: on the low frequency side ( 15 kHz) the speed is limited by the laser intensity. I present a model for the speed incorporating these effects that compares favorably with experiment. I present results of simulations of minority charge carrier concentrations in depletion regions. These exhibit self-similarity in space and time. The front of the concentrations follows a power law in time with an exponent that depends on the dopant concentration. Predictions from the power laws compare favorably with experiment.PHDApplied PhysicsUniversity of Michigan, Horace H. Rackham School of Graduate Studieshttps://deepblue.lib.umich.edu/bitstream/2027.42/140843/1/czarv_1.pd