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Micro/Nano Lithography

Micromanipulation using the backflow effect in liquid crystals

The flow of liquid crystals enables precise manipulation of hard-to-handle micro-objects such as microlenses and micromirrors.
16 July 2006, SPIE Newsroom. DOI: 10.1117/2.1200605.0235

The so-called backflow effect in liquid crystals (LCs) is the coupling between flow and directional change of LC molecules. In the past—for optical devices such as LC displays (LCDs)—this effect had the disadvantage of reducing contrast, which limited its application. But the advent of microfluidics has reactivated interest in LC flow. Indeed, LCs are proving to be an excellent matrix for microfluidic applications owing to our ability to control LC molecules by applying voltages to them.

Figure 1 illustrates the principle of LC flow. LCs are an anisotropic fluid composed of cylindrical organic molecules. Within a cell, LC molecules can be freely aligned by treating the substrate surface in a variety of ways. For example, coating the top and bottom electrodes with polymer layers and rubbing in parallel directions results in a state called the nematic π-cell. Applying voltage aligns the long axis of the LC molecules in the direction of the electric field, as shown in Figure 1(a). Switching the electric field off results in the relaxed state shown in Figure 1(b) and induces the flow represented by Uoff. Conversely, switching the voltage on reverses the state and generates a counterdirectional flow (Uon).

Figure 1. Flow inside a nematic LC π-cell provides a means of micromanipulation. (a) Activated nematic π-cell. (b) Inactivated nematic π-cell.

Using the backflow effect for micromanipulation required solving two problems: generating net flow without cancelling Uon and Uoff, and suppressing electrophoretic flow caused by ionic impurities.1 The problem of net flow was solved by changing the duty ratio, i.e., the duration of the on state, per cycle, of the applied rectangular wave in the case of nematic LCs,2 and by applying a sawtooth wave for ferroelectric LCs.3 The issue of electrophoretic flow was addressed by applying a high-frequency wave above 100Hz to prevent impurities from following the electric field.2,3Figure 2 shows the movement of a thin polyethylene film in a nematic π-cell using these techniques.

Figure 2. Photomicrographs track the motion of a thin film in a nematic π-cell. (a) The initial position of the film. (b) The position of the film 30s later.

In addition, we have succeeded in developing a two-dimensional (2D) micromanipulator (see Figure 3) using the twisted nematic (TN) cell, which is often used in LCDs. The principle of the 2D micromanipulator is illustrated in Figure 4. Alternating the states of Figure 4(a) and 4(b) generates the twisted flows Uon and Uoff, respectively: shown in Figures 4(c) and 4(d). Decreasing the duty ratio of the applied rectangular wave keeps Uon and Uoff from cancelling, and causes Uoff to predominate. Microparticles (spherical polystyrene beads) can then be introduced into this TN cell. Because the microparticles are naturally charged, they move in the z direction in response to electrostatic force. This movement is reversed by the polarity inversion of the applied voltage, as shown in Figure 4(b). Accordingly, changing the polarity of the applied voltage enables 2D (xy) manipulation. For example, the microparticles in Figure 3 were negatively charged, so positive polarity drove the particles in the +x direction. Conversely, negative polarity drove the particles in the +y direction.

Figure 3. These photomicrographs show the particle motion. (a) Positive voltage causes movement in the x direction. (b) Negative voltage causes movement in the y direction.

Figure 4. The scheme illustrates the principle behind the 2D LC micromanipulator. (a) Inactivated (off) TN cell. (b) Activated (on) TN cell. (c) Flow velocity distribution generated in the rising part of the rectangular wave. (d) Flow velocity distribution generated in the falling part of the rectangular wave.

Our techniques exploiting LC flow are suitable for precisely manipulating hard-to-handle micro-objects such as microlenses and micromirrors. We expect that, in future, these methods will also be applied to biochips and μ-TAS (micrototal analysis systems).

This research was partially supported by the Grants-in-Aid for Scientific Research for Young Scientists (B) (17760124) and Priority Area ‘System Cell Engineering by Multi-scale Manipulation’ (18048042) from the Ministry of Education, Science, Sports, and Culture of Japan.

Yoshitaka Mieda
Kochi University of Technology
Kochi, Japan
Yoshitaka Mieda obtained his PhD at the Tokyo Institute of Technology in 2003 and was a postdoctoral fellow at Toyota Technological Institute until March 2006. He is currently an assistant professor at the Research Institute of Kochi University of Technology. His research focuses on the application of soft matter to mechatronics.
Katsushi Furutani
Toyota Technological Institute
Nagoya, Japan
Katushi Furutani is an associate professor at Toyota Technological Institute. His research deals with applications of piezoelectric actuators and precision machining. He was a visiting associate at the California Institute of Technology in 1995 and a visiting associate professor at the Japan Aerospace Exploration Agency from 2004 to 2006.