Laser beam steering is the precise and controllable delivery of laser beams or other guided modes to a desired location. Image sensing, laser displays, and optical switches are examples of applications that utilize laser beam steering. Currently, laser beam steering is required in a broad variety of applications including optical displays, communications, biomedical imaging, space, battlefields, surveillances, and homeland security.
To accomplish laser beam steering, liquid crystals may be used. However, laser beam steering devices based on liquid crystals currently are expensive, have small apertures and dispersion problems, and steer over relatively narrow angles [1][2].
A micromirror is an optical semiconductor device that has a movable mirror plate. Micromirrors can also be used for laser beam steering applications. They may scan angularly in one dimension (1D) or 2D, and/or scan linearly, for instance, for phase control.
For endoscopic biomedical imaging, beam scanning devices with small size are crucial. However, existing laser beam scanning devices have small fill factors due to the large area needed for the actuation mechanisms. Small fill factors greatly increase the overall device size. This becomes a serious problem for intravascular imaging.
For air surveillance, large optical apertures are required. However, large mirrors tend to have very slow scanning speeds. In order to increase scanning speed, an optical aperture usually is partitioned into an array of a much smaller aperture, such as an optical phased array (OPA). In this case, the fill factor of the mirror array is a very important parameter since high-power lasers are usually used. If the fill factor is small, a large amount of power will be wasted. In addition, this ‘wasted’ power may hit on the actuators of the mirrors, which can damage the mirrors.
Existing micromirrors with high fill factors are currently made of thin-film microstructures. Consequently, their optical aperture sizes are small. Furthermore, thin-film Micro-Electro-Mechanical System (MEMS) mirrors tend to curl.
A variety of mechanisms that can be used for actuation in MEMS designs include electromagnetic, piezoelectric, electrostatic, and electrothermal actuation. Electromagnetic actuation requires external magnets, which complicates device packaging. Piezoelectric actuation typically achieves displacements on the order of a few microns. Electrostatically-actuated micromirrors can be difficult to scale up. In contrast, electrothermal actuation can generate large angular displacements.
Most micromirror designs are based on electrostatic actuation, which results in high driving voltages and small actuation ranges. The mirror portion of a micromirror is usually made from a reflective material such as aluminum. In one mirror actuation approach, each mirror is mounted on a yoke that is connected to two support posts by compliant torsion hinges. In this type of hinge, the axle is fixed at both ends and twists in the middle. Two pairs of electrodes control the position of the mirror by electrostatic attraction. Each pair has one electrode on each side of the hinge, with one of the pairs positioned to act on the yoke and the other acting directly on the mirror. Equal bias voltages are applied to both sides simultaneously to hold the mirror in its current position. A voltage difference applied to the two sides will generate angular scanning.
The electrothermal actuation approach for micromirror actuation has been demonstrated with rotation angles ranging from 30° to over 100° with mirror apertures of 1 mm to 3 mm. [3]-[8]. However, most of these micromirrors rotate about a hinge at the end of the mirror plate, so the optical center of rotation shifts during the mirror tilting. This center shift generates an optical phase delay and a lateral shift of the optical beam on the target. Furthermore, these mirrors have very small fill factors.
Embodiments of the present invention relate to a method and apparatus for high-fill-factor micromirror beam steering. Embodiments also pertain to a method of fabricating high-fill-factor micromirrors and micromirror arrays. Embodiments of the present invention can provide high-fill-factor micromirrors by hiding at least a portion of, and preferably the entire actuating engine underneath the mirror plate of each micromirror. In a further embodiment, the hidden actuators of the actuating engine can be located close to the center of the mirror plate such that a small displacement of the actuators can generate a large scanning motion of the mirror plate. Large aperture sizes can be implemented through making the mirror plate using single-crystal silicon. According to an embodiment, the actuators and the mirror plate can be made on a single substrate.
A micromirror according to an embodiment can include a micromirror plate formed of single-crystal silicon; a plurality of electrothermal actuators provided under the micromirror plate; and a pillar structure, wherein the pillar structure interconnects the plurality of electrothermal actuators to the micromirror plate.
In an embodiment, a method of fabricating a micromirror can include preparing a silicon-on-insulator (SOI) substrate: fabricating electrothermal actuators on a front side of the SOI substrate; and fabricating a micromirror plate on a back side of the SOI substrate, wherein an inner silicon region of the SOI substrate is removed except for a region providing a pillar structure interconnecting the plurality of electrothermal actuators and the micromirror plate. The front side of the SOI substrate can be bonded to an anchor substrate for mechanical support.
Embodiments of the present invention relate to a method and apparatus for high-fill-factor micromirror beam steering. Embodiments also pertain to a method of fabricating high-fill-factor micromirrors and micromirror array. According to an embodiment, the micromirror can have multi-degree-of-freedom motion control. In a farther embodiment, a large scanning range can be implemented. Advantageously, embodiments of the present invention can provide both a large scanning range and high fill factors. In one embodiment, process integration can be accomplished to fabricate the subject micromirrors without assembling multiple separate components.
According to an embodiment, at least a portion of, and preferably the entirety of the actuators for a micromirror can be located underneath the mirror plate. Accordingly, embodiments can provide high fill factors. In one embodiment, fill factors can be greater than 90%. In a specific embodiment, the fill factor can be limited by only the spacing between adjacent mirror plates because the actuators can be positioned completely below the mirror plates.
By making a mirror plate from single-crystal silicon (SCS), the mirror plate can be made flat and large. Accordingly, embodiments are capable of providing a large aperture size. The mirror plate can be coated with a metal, such as aluminum or gold, or can be coated with a multi-layer thin-film stack, such as a highly reflective multi-layer thin film stack.
By locating actuators close to the center of the mirror plate and below the mirror plate, a small displacement of the actuators can generate large scanning of the mirror plate. Accordingly, a low driving voltage can be used to provide a large angular scan range.
The subject micromirrors can be fabricated using an integrated process. For example, in one embodiment, the actuators and the mirror plate can be made on a single substrate. Then wafer-level or flip-chip bonding can be used to bond the substrate having the actuators and the mirror plate to a support substrate to provide mechanical support. In one embodiment, the support substrate can also provide electrical connections. The electrical connections may be provided by through-silicon vias. Advantageously, the integrated process of certain embodiments of the present invention can produce a high yield of devices.
Embodiments of the present invention can be used to provide a variety of high-fill-factor (HFF) products, including but not limited to HFF scanning mirrors; HFF vertical scanning mirrors; HFF microlenses; HFF micromirror arrays; HFF microlens arrays; HFF optical phased arrays; HFF micromirror-based optical imaging probes; and HFF microlens-based endoscopic imaging probes.
Large-aperture, tip-tilt-piston micromirrors can be difficult to make. Large-aperture micromirrors with large rotation angles are desired for certain laser beam steering applications. However, thin-film MEMS mirrors are generally not suitable for such applications because of their curling and small sizes. Advantageously, single-crystal silicon (SCS) based micromirrors can be employed in large-aperture micromirrors for flatness and robustness.
To increase scanning speed where a large optical aperture is needed, the optical aperture usually is partitioned into an array of much smaller apertures. In one embodiment, this array can be an optical phased array (OPA). An OPA is not a simple homogeneous micromirror array. Rather, in an OPA, each micromirror generates a phase shift such that the phase differences of the light from all the micromirrors will be only zero or multiple 2π (modulo 2π). In other words, each micromirror can simultaneously generate independently-controllable rotational and piston motion.
Embodiments of the present invention can provide a high-fill-factor and large-aperture tip-tilt-piston micromirror array. According to an embodiment, the high fill factor can be accomplished by locating the actuation engine at least partially, and preferably entirely, underneath the mirror plate. Electrothermal actuation can be used to obtain a large scan range. The electrothermal actuation can be accomplished through bi-layer, i.e., bimorph or multi-layer structures with materials having different coefficients of thermal expansion (CTEs). In one embodiment, the actuators can be inverted-series-connected (ISC) bimorph actuators. The ISC bimorph actuators can be used to achieve tip, tilt and piston scanning. Referring to
To obtain large rotation angles, the structure shown in
For one dimensional (1-D) rotation and piston motion, all four actuators can be first provided with equal currents. Then, in one example, for pure rotation, the current of Actuator-2 is increased while the current of Actuator-4 is decreased by the same amount. For pure piston, the currents of all four actuators are decreased or increased by the same amount.
In one embodiment, a micromachining process based on a silicon-on-insulator (SOI) wafer can be used to fabricate the device without assembling. The process flow according to an embodiment is shown in
Referring to
As shown in
At this point, the process can be continued at either wafer level or die level. The difference between the two cases is that the wafer-level processing uses wafer-to-wafer bonding while the die-level processing will add a dicing step and use flip-chip bonding. The following steps are the same for both cases. For either case, there are a variety of options. Two options in accordance with embodiments of the invention are illustrated: one is shown by
For the former option, as shown in
For the latter option (FIG. 3H′-3J′), as shown in FIG. 3H′, an isotropic silicon etch can be used to undercut the silicon 100a underneath the oxide/Al or Al/oxide bimorphs 107. Next, as shown in FIG. 3I′, a bonding (either wafer-to-wafer or flip-chip) can be performed. This can be accomplished using a carrier substrate 200 as described above. Finally, as shown in FIG. 3J′, the bonded assembly is flipped over and a silicon etch (anisotropic or isotropic) followed by a dry oxide etch can be used to release the mirror 108.
According to embodiments, to increase the fill factor, the actuators are located, or hidden, at least partially and preferably entirely, underneath the movable mirror plates, as shown in
where g is the gap between adjacent mirror plates, and b is the active mirror pixel size. For example, if g=0.1 mm and b=1 mm, then the fill factor will be 91%. If g=0.1 mm and b=5 mm, then the fill factor can be as high as 98%. According to embodiments, b can range from 1 mm to 10 mm and g can range from 10 μm to 200 μm.
Meanwhile, the size of the actuators is much smaller than the mirror plates along the rotation direction(s) such that the mirror plates have enough room to rotate. For instance, if the mirror plates rotate about y axis, then ax should be much smaller than b. If the mirror plates rotate about both x and y axis, then both ax and ay must be smaller than b. For instance, an HFF mirror array can be designed with hidden actuator size of (ax and ay) 800 μm and mirror size (b) of 2.45 mm, such that
are less than ⅓.
The actuators underneath the mirror plates can be anchored on a substrate.
Comparing these two embodiments, the embodiment of
Using frames as support (as the embodiments shown in
The geometric parameters of an ISC actuator are defined in
where aT is the difference of the CTEs of the material layers, and βρ is a parameter called the curvature coefficient. βρ is a unit-less parameter that varies from 0 to 1.5 and depends on the relative layer thicknesses and elastic moduli. With Lb=100 μm and tb=2 μm, the maximum tip displacement and tilt angle are about 50 μm and +/−15° at a 100° C. temperature change.
For optical phased arrays, the required vertical displacement is in the range of 10 μm, and the rotation angle is in the range of +/−15°. Accordingly, in one embodiment, the following parameters can be used: Length: Lb=90 μm; Bimorph thickness: tb=2 μm; Bimorph materials: Al and SiO2; and Heater material: Platinum.
An S-shaped actuator is half of an ISC actuator. The advantages of using single S-shaped actuators include the simplicity and larger scan range. The same geometric parameters for ISC actuators can be used for S-shaped actuators.
Five mirror embodiments with the mirror sizes ranging from 1 mm to 10 mm and five mirror arrays with the aperture sizes ranging from 5 mm to 12.5 mm have been implemented. A photomask set with all the embodiments has been made.
A device was fabricated using a 4 inch SOI wafer having 50 μm device thickness, 1.5 μm buried oxide thickness, and 400 μm handling layer thickness.
All patents, patent applications, provisional applications, and publications referred to or cited herein are incorporated by reference in their entirety, including all figures and tables, to the extent they are not inconsistent with the explicit teachings of this specification.
It should be understood that the examples and embodiments described herein are for illustrative purposes only and that various modifications or changes in light thereof will be suggested to persons skilled in the art and are to be included within the spirit and purview of this application.
The present application claims the benefit of U.S. Provisional Application Ser. No. 61/085,752, filed Aug. 1, 2008, which is hereby incorporated by reference herein in its entirety, including any figures, tables, or drawings.
The subject invention was made with government support under a research project supported by U.S. Air Force Grant No. FA9550-08-0292.
Number | Date | Country | |
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61085725 | Aug 2008 | US |