By Stefan Vorndran and Scott Jordan, PI, Physik Instrumente L.P.
Ever-increasing requirements for more precise motion control has forced manufacturers of piezoelectric positioners to find ways to overcome their limitations, such as travel range and linearity, while preserving the unmatched speed, reliability and resolution capabilities of piezoelectric devices.
Precision motion control in general, and nanopositioning in particular, is critical in many high-technology fields such as bio-nanotechnology, semiconductor test and measurement, optical alignment, nanoimprinting, scanning microscopy and microlithography. Choosing the right nanopositioning stage depends not only on resolution and accuracy, but also on factors such as dynamics, size, application environment, and cost.
A nanopositioning stage is a motion device capable of repeatedly producing motion in increments as small as a nanometer or less. There are several ways to achieve resolutions of one nanometer or below. Some may seem as simple as bolting a microstepped motor and a reduction gearbox to a leadscrew mechanism. More sophisticated approaches use additional position feedback in the form of an encoder and interpolator circuit. However, there is more to a nanopositioning system than a high-resolution motor.
Friction is the enemy
Friction leads to hysteresis and induces guiding errors such as tilt and wobble. In most positioning systems, guiding errors are not measured, and hence remain uncontrolled. Tilt, wobble and run-out errors automatically contribute to positional inaccuracy. This fact is often neglected and rears its ugly head when several individual positioners are combined into one multi-axis system.
Friction is also inherent in traditional motor/leadscrew drive mechanisms. Even though such drives have improved gradually over time and still provide many advantages for mainstream applications, the traditional approach is often not the answer in demanding applications such as optics, semiconductor and bio-nanotechnology fields. As the demand for speed and precision has continued to increase, motion control system manufacturers have had to develop better options to keep pace.
Piezoceramic drive systems have always been known for their fast response and atomic resolution, though at limited motion ranges. Progress in piezo mechanisms, as well as control technologies, has solved the travel distance/precision conundrum. Scientists and motion engineers now have access to a number of piezo systems with virtually unlimited travel, without giving up stability, precision and speed. (See the Quick Guide on piezo actuator technology on page xx for descriptions of these systems.)
Following are some motion control applications that have spawned the development of these new technologies.
Positioning and alignment systems in e-beam lithography systems and scanning electron microscopy (SEM) can be equipped with electromagnetic drive mechanisms. However, the expense to shield them and/or position them outside of the action is very high, along with the increase in size. Fieldless piezo ceramic motors are significantly smaller, and can be positioned anywhere inside of these machines without causing negative effects.
Medical technology can also benefit from piezo solutions that have been optimized over many years for applications in semiconductor manufacturing and testing, and biotechnology research. Active ceramic components, such as piezo ceramic sensors and actuators, have already been used in medical design technology; for example in micro-pumps, ultrasonic transducers, fast valves for nano-dispensing applications, and for laser beam control in eye and skin surgery.
For medical imaging applications, such as Magnetic Resonance Imaging (MRI) systems, ultra-high field imaging can have significant advantages for cardiac imaging. However, it turns out that tuning several coils in a whole-body scanner to achieve the best performance can be a lengthy process. Replacing the manual tuning with computer controlled non-magnetic piezo motors speeds up the process and provides better results at the same time, as shown in a recent paper by researchers at the Oxford Centre for Clinical Magnetic Resonance Research, Oxford UK, and the Center for Magnetic Resonance Research, Minneapolis.
3D-optical microscopy and Optical Coherence Tomography (OCT) can also benefit from piezo drives due to their high-efficiency, direct-acting linear motion, high-resolution, fast response and non-magnetic characteristics.
Small ranges but high throughput
In modern drug-discovery applications, a multitude of samples must be examined in the shortest possible time. Techniques such as fluorescence imaging are employed and require precise focusing on small amounts of liquid, usually held in multiwell plates, Figure 1.
For long range, well-to-well positioning, conventional electric motors or voice-coil drives typically provide the required speed and precision. However, the focusing is best achieved with frictionless, piezo flexure stages or objective positioners. Response times on the order of a few milliseconds allow extremely fast focusing and thus rapid data acquisition. The fast response also reduces the risk of photo bleaching caused by long-term exposure.
Similar speed/resolution requirements are prevalent in near-field scanning optical microscopy (NSOM). Here, small samples are scanned, typically 100 × 100 µm to 500 × 500 µm, with nanometer lateral resolution. To minimize the scanning time and achieve the high resolution required, flexure-guided piezo stages are the only option. The latest designs employ a parallel-kinematic motion principle, with all actuators acting on one moving central platform, greatly reducing inertia for much improved dynamics. Capacitive sensors integrated into the stage take multi-axis measurements against a common fixed reference (parallel metrology). This approach allows drift-free positioning with nanometer straightness—not available with classical stacked/nested multi-axis designs.
The same approach yields superior surface metrology results in atomic force microscopes (AFM). Progress in semiconductor development relies heavily on materials testing, and an AFM’s output data is only as good as the out-of-plane motion (OOPM) of the XY scanning stage it employs. Here, traditional bearings are totally out of the question and the requirements have been pushing the mechanical limitations of the best flexure designs. Active trajectory control approaches (compensating minute off-axis errors with integrated piezo transducers) now provide OOPM in the sub-nanometer realm, over large scanning areas to hundreds of microns, Figure 2.
Nanopositioning goes hybrid
Hybrid positioning systems combine the best of two worlds: long travel ranges with low power requirements and sub-nanometer resolution with very high dynamics. Progress in controller designs has made possible real-time closed-loop control of an actuator consisting of a piezo-flexure arrangement in series with a servomotor/ballscrew assembly.
In this example, the controller reads the stage position from an integrated, sub-nanometer-class linear encoder and continuously coordinates the piezoelectric and servomotor drives simultaneously in a way to provide the best possible overall performance, with rapid pull-in, nanometer-scale bi-directional repeatability and inherent axial stiffness. The actuator, Figure 3,has been proposed to drive the European Extremely Large Telescope (E-ELT)—a 39-m diameter next-generation telescope, segmented in 800 hexagonal mirrors. The combined motion of the frictionless piezo and the screw drive provides unprecedented smoothness and accuracy, even beating the required 1.7-nm RMS tracking precision. One has to consider, that under operating conditions the load on the actuator changes in a range of zero to 900 N. When the telescope tracks the stars, all 800 segments must stay aligned perfectly so as not to distort the wavefront of the incoming light. Under laboratory conditions, better than 0.8-nm RMS tracking accuracy was achieved, as was demonstrated in the white paper, “Piezo vs. Voice Coil Modules in the Hybrid Actuator for the E-ELT Telescope.”
High-force, piezo-walk linear motors
High-energy physics experiments often require components to be insensitive to strong magnetic fields and EMI. An ideal scenario for a motion control device would be to hold a position exactly when powered down. A new robust piezo motor based on the piezo-walk principle is now available to provide backlash-free, highly stable motion over centimeters of travel with nanometer resolution. Due to the self-clamping design, no power is dissipated in steady state, and a position can be locked into place even when the controller is powered off.
The piezo-walk principle is based on coordinated motion of several longitudinal and lateral piezo actuators arranged about a central ceramic runner. A digital controller sequences their operation, providing high-force, long-travel step-mode actuation plus picometer resolution high-bandwidth actuation. This type of piezo motor can generate forces to 170 lb, and is also vacuum-compatible and fieldless, with nanoscale power-off position stability for months.
Compact piezo walk motors can be integrated in low-profile linear translation stages, shown in Figure 4, such as those used in laser tuning and aligning applications. They combine long-travel motion with a highly dynamic short-range sweep mode.
Multiple piezo motors can be arranged to form compact hexapod 6-axis positioners, as seen on the lead page of this article. The hexapod approach, with its virtual pivot point and central aperture, is crucial for optical alignment problems as large as secondary mirrors in the latest generation earthbound telescopes, and as small as fiber-to-photonic-component-alignment in telecommunication chips.
Eliminating the travel/resolution tradeoff
Classical piezo flexure positioners excel through their frictionless, guiding systems, rapid response in the kHz range and extremely high reliability. Piezo flexure actuators have passed 100 billion cycles of life testing by NASA/JPL for the Mars Mission and are currently in use on the Curiosity rover. The motion of a piezo flexure actuator is roughly proportional to the applied voltage, often generated by a digital-to-analog converter (DAC) driving an amplifier.
In recent history, piezo flexure motion was limited to approximately 100 µm, but advances have pushed the limits to beyond the millimeter range. The number of addressable positions for such a piezo mechanism is 2b – where b is the bit-width of the DAC’s digital input. In order to cover longer travel ranges while maintaining nanometer resolution, DAC’s with more bits were the only solution. A patented technology called HyperBit now leverages the under-utilized time-domain capability of today’s DACs, converting it into up to eleven additional bits of physical positioning resolution. In a recent digital-based servo-control system for x-ray interferometers, 5 picometers (10 exp -12 m) positioning resolution was achieved using this novel technology.
High-accuracy position feedback is essential in a good nanopositioning system, and direct motion metrology is the preferred choice. Direct metrology measures motion where it matters most to the application. Examples of high-resolution, direct metrology sensors are capacitive sensors, laser interferometers and non-contact optical, incremental encoders.
Laser interferometers are capable of accurately measuring long distances and some provide sub-nanometer resolution, although bulky optics must be mounted onto the moving elements of the motion system.
Optical encoders are more compact and rely on diffraction between a moving reticle and a scale composed of finely pitched lines. Position is determined by counting fringes and interpolating between individual peaks, similar to interferometry. The latest linear encoders can provide resolution in the 100 picometer range. Interferometers and incremental optical encoders are relative position sensors that must be initialized at a reference position. The stability of this reference position also influences the overall precision. While not yet common, high resolution absolute encoders break the nanometer barrier but are still held back by high cost and more complex interfacing.
For travel ranges of less than 1 mm, capacitive sensors have emerged as the default choice. They are compact, high-bandwidth and absolute measuring devices providing sub-nanometer resolution. For less demanding applications, strain gauge sensors (piezoresistive sensors) are a good alternative.
Piezo-driven mechanisms achieve accuracy and repeatability by integrating position feedback sensors.
Piezoresistive strain gauge sensors (PRS) are economical, but are temperature-sensitive devices that are easily integrated in positioning devices. They are glued to the flexure structure or piezo stack, but the extra layer of epoxy between the sensor and structure makes it a challenge to get sufficient long-term stability. PRS do not measure distance directly, but infer position of the moving platform from the nanoscale warping of the structure, Figure 5. Due to the indirect measure of position, inaccuracies can occur and orthogonality errors are unobservable. Calibration to an interferometer allows them to achieve adequate accuracies for classical microscopy applications. Because their output signal is a low voltage dc current, the derived position can be more susceptible to noise pickup and drift.
Capacitive sensors are high-value sensors composed of diamond-machined plates that directly measure the absolute position of the stage platform, as shown in Figure 6. Traditionally deployed in high-end semiconductor manufacturing tools and advanced microscopy applications, such as single-molecule studies, capacitive sensors provide especially precise, accurate and fast position metrology. Because the stage platform is measured directly, cross-talk and orthogonality can be eliminated. And because no glue is used to attach the sensors to the platform, they are exceptionally stable and reproducible and are usually calibrated to 4th order or higher. Their tightly-controlled RF signal is consequently robust against noise. Their inherent stability makes them an ideal fine-positioning companion to ultra-stable piezo motor long-travel coarse-positioning stages.
Assessing the right nanopositioning option
Piezo ceramic motion systems have long been the number one choice for ultra-high precision motion. With ever-increasing requirements from the optics, biotech and semiconductor industries in recent years, manufacturers were forced to find ways to overcome limitations such as travel range and linearity, while preserving their unmatched speed, acceleration and resolution capabilities.
It is important to understand the user’s application, and its requirements on dynamics and precision, as well as the control and interfacing preferences of the user. Making the right choice in nanopositioning involves assessing multiple criteria. But if the user is willing to do a bit of research, and engage in a dialog with a credible manufacturer, the result will be a significant step forward from what was feasible just a few years ago.
Quick guide to different types of piezo motors and actuator systems
All piezo motors and actuators are intrinsically vacuum-compatible and non-magnetic.
A) Simple Piezo Actuators (Stack, Tube, Shear, Bender) — Expand proportionally to the applied voltage, travel range up to 0.2 % of actuator length.
• High force available, to thousands of kgs;
• Very fast response – microsecond to millisecond range;
• Frictionless, sub-nanometer resolution;
• Travel range typically 10 to 200 µm for stacked actuators; 3 – 4 mm for (low force) bender actuators;
• Closed-loop operation with feedback sensor for higher linearity.
• Stacked Actuators (most common): Available in cofired multilayer construction (typically 100 V); and classical design (stack of discrete PZT disks/electrodes, 500 to 1000 V). High force, motion typically up to 200 µm. Also available with aperture.
• Shear Actuators: Lateral motion, allows design of small, very fast XY and XYZ positioners, also used in piezo stepping motor designs. High force, travel typically limited to 20 µm.
• Tube Actuators: Often used in microdispensing (pump) applications and as scanner tubes for AFM microscopy. Very fast response (very low inertia), low force (fragile), travel range typically <20 µm. XY scanner tubes available.
• Bender Actuators: Available in multilayer construction (60 V); and classical (bimorph) design (200 to 1,000 V). Low force (< 1 kg), very long deflection (to several millimeters), relatively slow response (approximately 10 msec).
B) Piezo Flexure Actuators/Positioners (flexure-guided, piezo stack-driven nanopositioning and scanning stage or actuator) — These more complex systems use frictionless flexures and motion amplifiers to provide extremely straight and flat motion, and often longer travel than can be accomplished with simple piezo actuators. For the highest accuracy, integrated capacitive position sensors provide sub-nanometer precision in multiple degrees of freedom.
• Frictionless, fast response (0.1 to 10 msec), sub-nanometer resolution feasible; scanning frequency up to kilohertz range;
• Integrated multiaxis-systems available;
• Internal motion amplifier provides typical motion range up to 2,000 µm;
• Essential for nanoalignment, scanning optical microscopy and nanomanipulation;
• Position feedback sensor can be integrated (typically strain gauges for entry level, or capacitive for high-end systems and independent multi-axis measurements).
For A and B the motion is basically proportional to the dc output voltage of the piezo driver/servo controller. A position feedback sensor is required for linearization, due to the nonlinear behavior of piezo material.
The piezo actuators/motors use different types of controllers, and typically, incremental feedback sensors.
C) Ultrasonic Motors
• Based on high frequency oscillation of a piezo plate (stator) at the nanoscale;
• Oscillation is transferred to a slide or rotor via micro-friction;
• Unlimited motion range, high speed (to 1000 mm/sec in some of the latest designs), fast response (10 to 10s of msec);
• Resolution typically 10 to 50 nanometers. Forces, typically 2 to 10 N (0.5 to 2 lb.);
• Power-off, position-hold capability;
• Small amount of particle generation due to friction.
D) Piezo Stepping Motors (PiezoWalk) such as PI NEXLINE Drive.
• Virtually unlimited motion range;
• Based on accumulation of small highly controllable steps;
• Picometer resolution by means of direct piezo actuation (linear mode, dither mode);
• Compact and high force to 170 lb (for off-the-shelf units),
• Significantly lower speed than ultrasonic motors (1 to 10 mm/sec);
• Fast response (< 1 msec feasible), very high stiffness;
• Drift-free power-off, position-hold.
E) Piezo Inertial Motors (Stick-Slip Motors) — Very compact, motion-based on the stick-slip-effect.
• Most economical and compact design;
• For applications that require slow motion and low force;
• Challenging closed-loop control;
• Not recommended for applications that require constant velocity.
Physik Instrumente L.P.
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