Further details of the present invention are explained with the help of the attached drawings in which:
Embodiments of stage stacks in accordance with the present invention can be employed in several types of MEMS including probe storage devices, cell sorters, optical systems, and other devices. For example, a cell sorter wherein healthy and sick cells having different characteristics are caused to migrate due to stimulation. While stage stacks are described particularly with regard to probe storage applications wherein a media device is positioned relative to a plurality of contact probe tips, embodiments of stage stacks for forming micro-movers for still other applications are intended to be within the scope of the present invention.
Referring to
The movable plate 140 can be urged in the X-Y Cartesian plane by taking advantage of Lorentz forces generated from current flowing in a conductor when a magnetic field perpendicular to the X-Y Cartesian plane is applied across the conductor current path. Preferably, coils can be used in order to provide force for moving the movable plate 140. At least one coil 102 can be placed on the movable plate 140. In order to provide 2D motion of the movable plate the coils can be arranged in a cross configuration (as shown particularly in
Depending on application, movable plate 140 can perform different functions. For example, the movable plate 140 can be used to move objects, to store data, to reflect radiation, etc. Either one or both principle surfaces 106, 108 of the movable plate 140 can be used to perform the required function. The principle surface used to perform a required function is referred later as a functional surface of the movable plate 140. In some applications, presence of the coil on a functional surface of the movable plate is allowable. For example, if the micro-mover is used to move small objects and these objects are not affected by the voltage and the current in the coils 102 then the principle surface of the movable plate 140 with the coil can serve as a functional surface. However, in some applications presence of the coil on the functional surface is undesirable. For example, in probe storage devices the functional surface of the movable plate 140, preferably, is made very smooth to allow high-speed probe scanning and avoid damage of cantilevers and contact probe tips during scanning the memory media. Coil represents a profile on the surface and, therefore, if coils are located on the functional surface then the area occupied by the coils can not be used for storing data. In such applications coil can be located on the principle surface of the movable plate 140 opposite to the functional surface. In this case utilization of the surface of the movable plate 140 need not be affected by the coil layout. In other embodiments the coils can be formed on the functional surface of movable plate 140. In such embodiments, a portion of the surface of the movable plate 140 will be dedicated to the coils, reducing surface utilization of the movable plate.
The four coils 102 can be formed or otherwise disposed on a first surface of the movable plate layer 140 and can comprise multiple windings. Coils can be disposed on either one of principle surfaces 106, 108 of the movable plate (as shown in
The stage stack as shown has a tiered arrangement so that a portion of the bottom cap 110 and the plate layer 104 can include bond pads 180 on exposed surface of the corresponding component. Bond pads 180 are easily formed by well known semiconductor processes. The bond pads 180 enable electrical communication with circuits formed within the corresponding component. Electrical connections are made using wire bonding to the bond pads located on the stationary portion 120 of the plate layer 140 and on the bottom cap 110. In other embodiments, electrical communication can be achieved through some other structure, such as a vertical, conductive structure formed along a peripheral z-axis edge of the component.
A gap 121 can exist between the movable plate 140 and stationary portion 120 of the plate layer 104. The movable plate 140 can have a range of motion approximating the width of the gap 121 in any direction. The suspension structure 150 further suspends the movable plate 140 at a substantially uniform distance from the bottom cap 110 (i.e. without substantial out-of-plane shift or bending). The distance between the movable plate 140 and the bottom cap 110 can approximately correspond with a distance between the stationary portion 120 of the plate layer 104 and the bottom cap 110, which can be defined by a thickness of a bond ring 182 disposed between the stationary portion 120 and the bottom cap 110 for causing the stationary portion 120 and the bottom cap 110 to be fixedly connected.
Electrical components, for example IC circuits, (not shown in
The top cap 130 is fixedly connected with the stationary portion 120 of the plate layer 104 by way of a bond ring 182 or set of bond rings. The volume between the bottom cap 110 and the top cap 130 within which the movable plate 140 is entirely disposed can be hermetically sealed to prevent contamination and interference with the movement and operation of the movable plate 140 and/or structures adapted to interact with the movable plate 140. The bottom and top caps 110, 130 provide mechanical and environmental protection of the movable plate 140. The bottom and top caps 110, 130 are bonded to the plate wafer 104 at the wafer level. Preferably, hermetic wafer bonding process is used. The wafer bonding process, preferably, allows the transfer of electrical signals between the plate layer 104 and the caps. The bonding gap between the movable plate 104 and the caps is small and well-controlled by the wafer bonding process. As described in further detail below, a thin layer of gas between the movable plate 140 and the caps 110, 130 can provide dampening of vertical motion of the movable plate 140 due to a squeeze film effect.
Referring to
In some embodiments, the cap wafer 132 can comprise small-area stops 197 extending within the cavity 194 for resisting vertical and/or rocking motion of the movable plate 140. The small-area stops 197 further reduce a risk that the movable plate 140 will adhere or contact a surface of the top cap 130. Preferably, the small-area stops 197 are located near the periphery of the cavity 194, although optionally one or more small-area stops 197 can extend from approximately the center of the cavity 194. The number of small-area stops 197 can be limited, for example to four or five in number, while satisfactorily resisting sticking of the movable plate 140 to the top cap 130. The movable plate 140 does not contact the small-area stops 197 under normal operation conditions, but rather contact occurs during shock events. It is estimated that a top cap 130 having four stops disposed along the periphery of the cavity 194 can expect to experience contact between the movable plate 140 and one or more small-area stops 197 when a rocking motion occurs, while expecting contact between the movable plate 140 and substantially all of the small area stops 197 when the micro-mover is loaded by a vertical acceleration. In other embodiments, small-area stops can be located on the movable plate 140 in substitution of, or in addition to small-area stops 197 extending from the top cap 130.
Multiple different bonding techniques can be employed to fixedly associate the top cap wafer 132 with the plate wafer 104. The bottom and top caps 110, 130 are preferably bonded to the plate wafer 104 at wafer level using low-stress, low-temperature bonding. At least some bonding techniques require the presence of bonding material on both the top cap wafer 132 and the plate wafer 104 (e.g. thermo-compression bonding, solder bonding). In still other bonding techniques, bonding material need only be deposited on one of the top cap wafer 132 and the plate wafer 104 (e.g. polymer bonding, adhesive bonding, bonding with frit glass, bonding with help of eutectic compositions). Where bonding material is deposited on both the top cap wafer 132 and the plate wafer, the bonding material can be patterned to help ensure alignment of the first and second bonding material. Preferably, a bonding pattern comprises one or more bond rings 182 (two as shown in
Optionally, the top cap wafer 132 can further include dicing grooves 196. The dicing grooves 196 are arranged so that bonding pads of one or both of the stationary portion 120 of the plate layer 104 and the bottom cap 110 are exposed when processing electrical connections is desired. The use of dicing grooves 196 can simplify the process of removing a part of the top cap wafer 132 without undesirably damaging metal lines and/or the bond pads of an underlying wafer, access to which is desired. These removed parts are also referred to herein as “pad expose cuts”. Optionally, additional grooves can be formed along the saw lines, simplifying dicing of the wafer stack during processing.
Still further, in some embodiments it can be desired that one or more dead stops 198 extend from one or both of the top cap wafer 132 and the plate wafer 122 for controlling a height of a bonding gap between the wafers. During bonding, the bonding material can experience squeezing due to one or more of softening, melting, or otherwise undergoing a change in rigidity, combined with pressure applied to the stack of wafers. The bonding gaps between the cap wafers and the plate wafer can decrease until a physical limit is reached with the dead stops 198 contact an opposing surface. The bonding gap can be fixed in relative position when the physical limit is reached. The bonding gap height is thus determined by the height of the dead stops 198.
A target bonding gap between the wafers can be small, depending on the application for which the micro-mover is used. In some embodiments a height of the one or more dead stops 198 can have a range as small as 0.5 um to 2 um. The one or more dead stops 198 can be formed using myriad different techniques. One such technique for forming dead stops 198 having a precise height employs semiconductor processing to form dead stops 198 out of a thin film layer or a stack of thin film layers. For example, dead stops 198 can be formed from thermal oxide. The thickness of a thermal oxide film can be controlled with nanometer-range accuracy.
Referring to
Referring to
Electrical components, for example IC circuits, (not shown in
If coils 102 and electrical components are formed on the second principle surface of the stationary portion 120 of the plate layer and the movable plate 240 then it can be desired that some of the electrical lines (not shown in
Referring to
A coil having n turns will generate a maximum actuator force, Fpeak, according to the equation:
F
peak
≧I
max
·B·n·l
active
where B is the average magnetic field in the active areas, Imax is the maximum current in the coil and active is the average length of the active segment generating the force. The above formula assumes that magnetic field B has the same average magnitude and opposite directions in active areas 1 and 2. Preferably, the maximum actuator force should be at least as sufficient as the minimum force required to achieve the required maximum displacement at a desired maximum acceleration.
The maximum acceleration of the movable plate provided by the actuator is:
where Mplate is the mass of the movable plate, ρSi is the density of silicon, λ·Lplate·Wplate is the area of the movable plate with Lplate and Wplate corresponding to the length and width of the movable plate and λ is a coefficient corresponding to the portion of the movable plate less the suspension arrangement.
Power dissipated by the electromagnetic actuator, i.e. by the coils 102, is another important parameter of the micro-mover. Some application can have either peak power or average power limitations or both. For example, using micro-mover in the portable devices can put some limitations of the power dissipated by the micro-mover. The peak power Ppeak dissipated by one coil is equal to:
where ρcoil—resistance of the coil material; lcoil, wcoil, and tcoil—length, width, and thickness of the coil wire, correspondingly.
Bending of the movable plate due to bimetallic effect caused by the presence of the coil and some dielectric layers on the movable plate should be considered in some micro-mover applications, for example, in probe storage devices. An increase in an amount of metal on the movable plate can cause an increase in bending of the movable plate.
Coil design can be affected by the maximum current density allowable in the coil and/or by the maximum power that can be dissipated by the micro-mover. Coil design can benefit from accounting for one or more of the following parameters:
For applications where bending of the movable plate due to bimetallic effect is not important, it can be desirable to increase both the thickness of the coil metal as well as the width of the coil wire and number of turns. Preferably, a cross-section of the coil can be chosen roughly the same as a cross-section of a metal line connecting the coil with the stationary portion.
In applications where bending of the movable plate due to bimetallic effect can be a limiting factor, the amount of metal can be problematically increased where one or more of the width wcoil or thickness tcoil of the coil wire is increased, or where an average length 1average of the turn is increased. Given the equation:
where A is a coefficient, which does not depend on coil wire width and thickness, but depends on coil and plate geometry and working temperature range; and δmax is the maximum allowable bending of the movable plate, it is possible to determine a geometry of a coil that produces a bending of the movable plate within the desired tolerance. If flatness of the movable plate is a concern, then thickness of the movable plate should be significantly larger than a thickness of the coil. A minimum thickness tSi of the movable plate for a given coil design can be defined to satisfy bending requirements given a geometry of the coil and the following formula:
Maximum actuator force can be increased by increasing one or both of a thickness of the coil, tcoil, and a product of the number of turns n and the width of the coil wire wcoil. However, a corresponding increase in the plate thickness tSi can result in an increase in suspension stiffness. Suspension flexures can have substantially the same thickness as the plate wafer from which they are is formed. A bending stiffness of the suspension arrangement in the direction of actuation is directly proportional to the thickness of the movable plate. Some micro-machining process techniques (e.g. reactive ion etching (RIE)) can limit an aspect ratio of the suspension flexures (flexure thickness to width ratio) obtainable with satisfactory reproducibility. The bending stiffness of the suspension is proportional to the third power of the width of the suspension flexure. Therefore, increasing the thickness of the movable plate can cause at least a linear increase in the bending stiffness when the width of the suspension flexure is maintained. If the width of the suspension flexures is increased proportionally to the thickness of the movable plate, the bending stiffness of the suspension is increased proportionally to the fourth power of the thickness of the movable plate.
There are two competing factors affecting the maximum acceleration of the movable plate due to an increase of cross-section of the coil wire: (a) a decrease in coil resistance tends to increase coil current and actuator force and, therefore, maximum acceleration; and (b) an increase of movable plate thickness increases mass and decreases the maximum acceleration provided by the actuator decreases. After reaching the limit of the plate bending, a further increase of the width of the coil and number of turns in the coil, as well as an increase in thickness of the coil does not provide an increase of the maximum acceleration due to an increase in mass of the movable plate. One coil design option is based on using such cross-section of the coil wire that carries the maximum allowable current density when the maximum voltage is applied to the coil.
As mentioned above, in some applications of micro-movers it is beneficial to use a two-stage actuator. A coarse actuator can be used for one or both of large displacements (in the range of microns or tens of microns) and relatively fast acceleration of the movable plate. A fine actuator can be used for achieving sub-nanometer positional accuracy and/or resolution. For example, if a stiffness of the suspension arrangement is 20 N/m and a coarse actuator utilizing two coils with n=14 turns with average active length of (active=6 mm, having the maximum coil current of 10 mA is used in a magnetic field of B=0.4 T then the coarse actuator can provide the maximum force of approximately 0.67 mN and the coarse actuator is capable of providing movable plate displacement of about 33 μm. A fine actuator consisting of a wire with an active length of 6 mm and maximum current of 1 mA can provide a maximum force of 2.4 μN, which is capable of providing movable plate displacement of about 120 nm. Assuming that the coarse actuator current is controlled within ±10 mA by a 12-bit DAC, its least significant bit (LSB) corresponds to about a 5 μA current increment and about 16 nm displacement increment. The fine actuator controlled by a 10-bit DAC has LSB corresponding to 2 μA current increment and 2.4 Å displacement increment.
The actuator of the micro-mover can be completed by a magnetic field generated at least across the coils 102. For example, the magnetic field can be generated by a permanent magnet associated with one or both of the top cap 130 and the bottom cap 110. The permanent magnet can be integrally formed with the corresponding micro-mover die structure 110, 130, or alternatively can be affixed to the corresponding structure 110, 130. Lorentz force generated by the coil current in a magnetic field is used to urge the movable plate 140 within the X-Y Cartesian plane relative to the stationary portion 120. Alternatively, the permanent magnet can be integrated with the parts of the package. Referring to
Where the micro-mover is employed for probes storage applications, there is a possibility that a write current could disturb the movable plate due to undesirable Lorentz force. However, for probe storage devices having media devices comprising phase change material, polarity dependent material, or other material requiring similar or smaller write currents to induce changes in material properties, movable plate movement due to write currents can be sufficiently small as to be within track following tolerance. In some embodiments, it can be desired that electrical trace layout be configured to generally negate the current applied to the contact probe tip, thereby minifying the affect.
It can be desirable to dedicate as large a portion of the movable plate as possible to application utilization (e.g. probe storage devices). To achieve increased utilization it can be desired to reduce the percentage of the movable plate area dedicated to a support structure and/or suspension arrangement. If a suspension arrangement of the movable plate suspension requires significant area, the area utilization of the device will be correspondingly limited. A movable plate that is movable is susceptible to damage from dynamic events such as shock and vibration. Embodiments of suspension arrangements and movable plate in accordance with the present invention can increase utilization while improving shock response.
Referring to
The suspension arrangement 150 can be built by patterning and etching the plate wafer 140 using a deep RIE etcher. In a preferred embodiment, the suspension arrangement 150 can include flexures having height to width aspect ratios of 10:1. An example of flexures can be one having a width of 13.8 um and thickness (corresponding to a thickness of the movable plate) of 136 micron. Prior art flexures for use in electrostatic actuators and other movement devices typically include aspect ratios of 40:1. A smaller aspect ratio can reduce the relative suspension stiffness variation during manufacturing, decrease dynamic performance variation and increase yield.
The suspension arrangement 150 provides very high shock tolerance. Further, the mutually perpendicular flexures allow substantially isolated motion within the X-Y Cartesian plane while reducing cross-coupling. The rotational stiffness of the movable plate 140 can be adjusted by changing the spacing between flexure pairs. Narrow flexure spacing produces a lower rotational stiffness while wide flexure spacing produces higher rotational stiffness. The suspension arrangement of
Combining the suspension arrangement 150, coils disposed on one of the principle surfaces, memory media disposed on the other principle surface of the of the movable plate 140 and the described above magnetic circuit allows probe storage device with high area utilization. For example, on a 10 mm by 10 mm stage, the effective area utilization is expected to be close to 70%. Such a high rate of area utilization can allow for high capacity with a small package as compared to prior art designs of probe storage devices.
Referring to
The present invention is not intended to be limited to suspension arrangements and/or movable plates as shown in the figures included herein, but rather the present invention is meant to include myriad different embodiments employing the underlying principles for arranging a movable plate as desired. One of ordinary skill in the art will appreciate the myriad different arrangements of flexures for movably connecting a movable plate with a stator such as a stationary portion.
Coils and possibly some other electrical components located on the movable plate can be connected to the stationary portion. Electrical connections can be made by placing metal lines on one or both sides of suspension flexures or by using additional flexible structures connecting the movable plate and the stationary portion. Where the metal lines providing the electrical connections are disposed along the suspension flexures it can be desirable to reduce out-of plane bending of the suspension flexures caused by metal disposed along the suspension flexures. Out-of-plane bending can be reduced by one or more of decreasing a cross-sectional area of the metal lines routed along the suspension flexures, disposing one or more dielectric layers between the metal lines and the body of the suspension flexures to compensate for out-of-plane bending that would otherwise result from metal lines due to the bimetallic effect, or placing metal lines both on the top and bottom of the suspension flexures.
In some embodiments, suspension flexures can be free of metal and minify an amount of dielectric deposited on the suspension flexures. Electrical connections between the movable plate and the stationary portion can be made with additional flexible structures. The additional flexible structures can comprise metal lines deposited on top of additional silicon flexures having a thickness substantially similar to the thickness of the movable plate. However, bending stiffness of the bridge structures can be made significantly smaller than bending stiffness of the suspension flexures. Alternatively, the additional silicon flexures can have a thickness smaller than the thickness of the movable plate so that the bending stiffness of the bridge structures is significantly smaller than bending stiffness of the suspension flexures. Alternatively, metal lines only or metal lines disposed over a dielectric layer can be employed having small X-Y bending stiffness.
In still other embodiments, number of bridge structures used for electrical connections between the movable plate and stationary portion can be reduced by using the substrate as a common electrode for some electrical components. For example, the substrate can be used as a ground electrode or as an electrode with the highest potential.
A thickness of the plate layer can be determined based on a plurality of factors including satisfying flatness requirements related to bimetallic bending and built-in stress associated with wafer processing, and enabling movement of the plate wafer through all steps of the fabrication process. Preferably, both the plate wafer and the suspension arrangements are fabricated from a stress-free material, for example, monocrystalline silicon. Using a stress-free material can ensure that the plate layer and suspension arrangement do not bend due to a stress gradient in the material in an equilibrium position.
As discussed above, the maximum allowable bimetallic bending of the plate wafer can be a limiting factor for the maximum acceleration of the movable plate provided by the electromagnetic actuator and, therefore, limit the speed of the micro mover. There are two components of plate bending. The first one is initial bending of the plate at a reference temperature, for example, at room temperature. The second one is related to an additional bending (or flattening) of the plate in the working temperature range. Improvement in micro mover bending performance can be achieved by thickening silicon in the areas of the movable plate that are disposed beneath metal, for example metal layer used to form coils, and thinning silicon in the areas of the movable plate that are not disposed beneath metal. Local thinning of the plate can be achieved using different etching techniques. For example, dry etching process can be used for thinning of the plate.
Some illustrative examples of movable plate cross-sections are shown in
Referring to
In still further embodiments, bimetallic bending of the movable plate can be reduced by employing a film stack in which thermo-mechanical stress is partially or mostly compensated due to selection of materials having different thermal expansion coefficients (TCE) and deposition conditions.
Patterning of materials deposited on the movable plate allows further decrease of plate wafer bending.
In other embodiments, materials other than thermal oxide can be used for compensation of movable plate bending due to metal features. For example, such materials can include plasma enhanced chemical vapor deposition (PECVD) silicon dioxide, PECVD silicon nitride, low pressure CVD (LPCVD) silicon nitride, and LPCVD silicon oxy-nitride. A compensation layer can be deposited at an elevated temperature, and the TCE of the material used as a compensation layer can be smaller than the TCE of silicon in the temperature range between the deposition temperature and room temperature. In still other embodiments, multiple different compensation layers can be employed to compensate for movable plate bending caused by metal features.
In some embodiments, one or more compensation layers can be deposited on the opposite (with respect to the coils) side of the movable plate. This option can enable flexibility both in the microstructure design and in the process design. To compensate for bimetallic bending of the plate due to presence of the coils the compensation layer on the opposite side of the plate can be deposited at an elevated temperature, and the TCE of the material used as a compensation layer can be larger than a TCE of silicon in the temperature range between the deposition temperature and room temperature.
The flatness of a movable plate can vary over a range of operating temperature. For example, if coils comprising copper are disposed on the back side of a movable plate comprising silicon, the differential thermal expansion between the silicon movable plate and the copper coils can cause the movable plate to bend out of plane, potentially beyond a required flatness tolerance (e.g. 1 μm). To reduce the out of plane bending, an SOI structure can be employed having a thermally grown oxide layer buried within a stack forming part of a media stage. The coils can be formed over a thin LPCVD oxide layer. Subsequently, the wafer is thinned until the buried oxide layer is exposed. The thermally grown oxide deposited at an elevated temperature will tend to cause the media stage to bend in a first direction such that the surface of the movable plate has concave shape. However, since the copper coils can be deposited on the opposite side of the stack at a temperature, which can be close to room temperature, the differential bending caused by the coils causes the movable plate to bend in a second, opposite direction. The net result is that the flatness of the movable plate remains within tolerances over a desired temperature range.
In general, structures comprising a metal deposited at a low temperature (e.g. electroplated metal) can be more difficult for compensation of bending of the movable plate due to small initial bimetallic bending of the movable plate combined with the large temperature dependence of the bending due to a difference in TCE between metal and silicon. The compensation layer(s) should have approximately the same bending characteristics, but opposite signs of temperature dependence. Deposition of compensating layers on both sides of the movable plate can be used for compensating of bending induced by a coil metal deposited at low temperature.
The stiffness of the suspension arrangement can determine the required maximum actuator force for a required range of movable plate displacement and for a required maximum acceleration. Preferably, the suspension arrangement is formed using deep reactive ion etching (deep RIE)—a process that allows forming profiles with near vertical walls. Deviation of suspension flexure side walls from verticality can affect the stiffness of the suspension arrangement. The larger the required etching depth, the thicker the suspension flexure should be in order to maintain small relative variation of suspension stiffness. It is desirable to have an aspect ratio of the suspension flexures below 25:1 and, preferably, below 10:1 to ensure good reproducibility of suspension flexure profile and suspension stiffness. The stiffness of a suspension flexure is proportional to the cube of its thickness in the direction of bending, and directly proportional to the width of the flexure. Therefore, maintaining the same aspect ratio for suspension flexures can cause increased stiffness of the suspension arrangement for lateral bending proportional to the fourth power of movable plate thickness. Correspondingly, both required actuator force and actuator power consumption rapidly increase with increase of plate thickness.
Preferably, thinning of the plate wafer is done after bonding of the plate wafer to the cap wafer. This option allows avoiding processing and handling of thin wafers. Different bonding patterns can be used in different applications. However, it is highly desirable to minimize the area occupied by the bonding layer because it may cause built-in stress and bending of the wafer stack, which later will be transferred into thickness non-uniformity and initial bending of the movable plate and suspension arrangement. Thinning of the bonded stack of the plate wafer and the cap wafer can be performed using standard grinding and/or polishing steps (e.g. chemical-mechanical polishing (CMP)).
In some applications, the flatness of the plate layer is more relevant. For example, fabrication of some probe storage devices can require a nanoimprinting step, which, in turn, can require a very high flatness of the plate layer. However, the plate wafer is bonded to the cap wafer only in some areas (bond rings). Therefore, when the stack of plate and cap wafers is loaded with some force during wafer thinning steps this load causes vertical deflection of unsupported areas in the plate wafer. As a result, flatness of the plate layer achieved after wafer thinning can be compromised. Flatness of the plate layer after thinning can be improved by using some number of supports for the movable plate as shown in
Supports 688 should be disconnected with the movable plate 640 in order to allow motion of the movable plate 640. This can be done at the same time that the suspension arrangement 150 is defined by etching through the plate wafer. Posts 687 shown in
Besides getting low bending of the movable plate, as it was discussed above, using SOI wafers as initial material for the plate wafers can be beneficial for achieving both uniform thickness of the plate layer and very high quality surface of the plate.
During etching of silicon 142, the buried layer 141 of silicon oxide will be exposed non-uniformly. Both some non-flatness of the wafer stack and some surface roughness after silicon etching step can be related to difference in silicon dioxide etching time in different areas. In order to eliminate this source of non-flatness and roughness it is possible to strip off silicon dioxide as well (as shown in
As described above, the micro-mover can be subjected to mechanical shock and/or vibrations. A thin layer of air between the cap(s) and the movable plate provides squeeze film damping of out-of-plane motion of the movable plate. It can be desirable to maintain a small air gap between the movable plate and one or both caps to achieve a desirable effect of squeeze film damping. In an embodiment, a height of the air gap between the cap and the plate is in the range of 1-30 μm. In some areas of the stack, an air gap can be taller to allow some out-of-plane motion of the movable plate and/or the suspension arrangement while avoiding mechanical contact with one or both of the cap wafers. Further, as mentioned above, small area stops can be formed either on the movable plate or in the recess on the cap wafer in order to allow mechanical contact between the plate and the cap wafer for shock protection.
In some embodiment, it can be desirable to include wide gaps around the suspension flexures to protect the suspension arrangement during shock events. Free motion of long and compliant L-shaped flexures shown in
In order to provide control of the motion of the movable plate it can be beneficial to maintain the main resonance frequency of the movable plate within a desired range. The resonance frequency is proportional to the square root of the ratio of suspension spring constant and mass of the movable plate. Therefore, the main resonance frequency can be controlled by changing either spring constant of suspension or by changing mass of the movable plate.
In some cases mass of the movable plate can be decreased by micromachining the movable plate from the coil side, as described above in reference to
Position Sensing
A position of the movable plate relative to a cap wafer and/or the stationary portion can be determined using position sensors. Myriad different techniques for determining position can be employed, including use of capacitive sensors, Hall-effect sensors, and temperature sensors.
Capacitive sensors for use in determining a position of a movable plate can comprise an electrode fixedly connected or integrally formed with the movable plate and an electrode fixedly connected or integrally formed with one of the top cap and the bottom cap. The electrodes of the capacitors should be shaped to provide a change in capacitance due to a motion of the movable plate in at least one direction. Referring to
With no out-of-plane motion (e.g. rocking motion) of the movable plate, there are four independent variables defining mutual position of the electrodes: X and Y displacement within the Cartesian plane, Z separation and an angle of rotation within the Cartesian plane. Four position sensors can be used to measure the values of the four independent variables. However, the movable plate can exhibit out-of-plane motion, such as rocking or shocks. In such circumstances, opposite edges of the movable plate may have different Z-displacement as a result of the out-of-plane motion. At least two additional position sensors can be implemented to obtain information about rocking motion of the plate. One of the sensors can be used for evaluation of rocking motion in X-Z plane and another sensor can be used for evaluation of rocking motion in Y-Z plane. At least six sensors can be used in such an implementation.
Referring to
Referring to
In alternative embodiments, micro-mover can have larger number of capacitive sensors. In particular, pairs of capacitive sensors sensitive to the same type of motion (lateral (X), transverse (Y), X-Y skew or others) can be implemented in such a way that output signal of the first sensor is close to zero level and the output signal of the second sensor is close to its full scale output when the movable plate is in equilibrium position. When the movable plate is in an extreme position then output signal of the first sensor is close to its full scale output and the output signal of the second sensor is close to zero.
In alternative embodiments, Hall-effect sensors sensitive to magnetic field can be used to determine the position of the movable plate. Hall-effect sensors measure position based on changes of the mobility of carriers in the presence of magnetic field. Hall-effect sensors can be employed in a micro mover, for example, in the form of magneto-resistors or magneto-transistors. Hall-effect sensors can be arranged in areas of the movable platform where a component of the magnetic field has its largest gradient. Areas with large gradients of magnetic field exist in the middle of the coils where the magnetic field changes polarity. Displacement of the movable plate causes changes in the magnetic field created by stationary magnets and can be detected by the Hall-effect sensors.
In still further embodiments, thermal position sensors can be used to determine the position of the movable plate. Myriad different types of thermal sensors can be employed. For example, a thermal position sensor containing a heater and a differential pair of temperature sensors can be employed. In one embodiment, a stationary heater (e.g. a resistive heater) can be formed on one of the cap wafers, and two temperature sensors can be connected with the movable plate and located symmetrically with respect to the heater so that in a neutral position a differential signal from the pair of temperature sensors is small. When the movable plate is urged away from a neutral position the distance between the stationary heater and one of the temperature sensors increases. Correspondingly, the distance between the heater and the other of the temperature sensors decreases. The temperature difference resulting from this movement causes an electrical signal proportional to the displacement of the movable plate.
Similarly to capacitive position sensors at least four magnetic or temperature sensors can be employed in order to measure displacement of the movable plate within the Cartesian plane and the angle of rotation of the movable plate within the Cartesian plane. At least two additional sensors can be employed in order to measure rotation of the movable plate in X-Z and Y-Z planes.
Electrical connections to the movable plate may require use of bridges. It is desirable to minify the use of bridges; therefore, it can be advantageous to employ position sensors requiring the smallest number of electrical connections between the movable plate and the stationary portion. Capacitive sensing allows electrodes located on the movable plate to be connected with the substrate, which can act as a common electrode. The substrate potential can be set to ground or to the high potential. Connecting capacitor plates to the substrate creates parasitic capacitors between the substrate and the stationary portions. In order to reduce the parasitic capacitance the movable plate can be micro-machined between the fingers of the electrodes. Shallow cavities in the areas between the fingers can reduce parasitic capacitance.
Another approach illustrated in
Hall-effect and temperature sensors require at least two independent connections per sensor. Further, temperature sensors utilizing heat transfer through the air between the heater and the sensors may be less accurate than Hall-effect sensors and capacitive sensors. Resolution provided by Hall-effect sensors and capacitive sensors is expected to be better than that of thermal sensors. Still further, capacitive sensors have certain advantage related to low power consumption in comparison with the magnetic and temperature sensors.
Fabrication of a Micro-Mover Having One Cap
Referring to
Referring to
Referring to
Referring to
Referring to
Referring to
Cuts 196 through the cap wafer 132 should be formed to remove portions of the cap wafer 132 and provide access to the bond pads 180 formed on the stationary portion 120. After release etching the microstructure can be fragile; therefore, the wafer stack can be mounted on a temporary carrier 185, as shown in
In alternative embodiments, it can be desired that pad expose cuts and dicing be performed before release etching of the movable plate 140, thereby further resisting contamination and/or damage to the movable plate 140. In such embodiments, release etching is performed at chip level, rather than wafer level. However, with an appropriate carrier the micro-mover can be batch processed. Such methods can eliminate use of a temporary carrier.
Fabrication of a Micro-Mover For a Probe Storage Device
Probe storage devices enabling higher density data storage relative to current technology can include cantilevers with contact probe tips as components. Such probe storage devices typically use two parallel plates. A first plate (also referred to herein as a contact probe tip stage) includes cantilevers with contact probe tips extending therefrom for use as read-write heads and a second, complementary plate (also referred to herein as a media stage) includes a media device for storing data. Motion of the plates with respect to each other allows scanning of the media device by the contact probe tips and data transfer between the contact probe tips and the media device.
In some probe storage devices, for example utilizing phase change materials in a stack of the media device, both mechanical and electrical contact between the contact probe tips and the media device enables data transfer. In order to write data to the media device, current is passed through the contact probe tips and the phase change material to generate heat sufficient to cause a phase-change in some portion of the phase change material (said portion also referred to herein as a memory cell). Electrical resistance of the memory media can vary depending on the parameters of the write pulse, and therefore can represent data. Reading data from the memory media requires a circuit with an output sensitive to the resistance of the memory cell. An example of one such circuit is a resistive divider. Both mechanical and electrical contact between the contact probe tip and the media device can also enable data transfer where some other media device is used, for example memory media employing polarity-dependent memory.
The media device can include a continuous recording media, or alternatively the media device can be patterned to define discrete memory cells having dimensions as small as approximately 40 nm or less. A contact probe tip can access a portion of the surface of the media device, the portion being referred to herein as a tip scan area. The tip scan area can vary significantly and can depend on contact tip probe layout and/or media device layout. For purposes of example, the tip scan area can approximate a 100 μm×100 μm (10,000 μm2) portion of the surface media device. To enable the contact probe tip to access substantially the full range of the tip scan area, the contact probe tip stage can move within the tip scan area and the media stage can be fixed in position. Alternatively, the contact probe tip stage can be fixed, and the media stage can move within the range of the tip scan area. The moving stage moves in both lateral (X) and transverse (Y) motion to traverse the tip scan area. Alternatively, both the contact probe tip stage and the media stage can move in a single direction, with one stage moving along the X-axis and the other stage moving along the Y-axis.
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In some embodiments, a lubricant can be formed on one or both of the media stack located on the movable plate and on the tips so that a restrictive frictional force between the array of tips and the movable plate 140 is sufficiently reduced.
Optionally, it can be desired that the contact probe tip wafer 212 be thinned to accommodate package specifications. For example, some standard packaging options for memory chips require memory chip thickness to be below 0.5-0.8 mm. Therefore, thinning of the stack of wafers may be appropriate for some memory applications. However, for systems in which probe storage devices replace hard disk drives, or other relatively bulky memory media, a memory chip need only be required to have a memory chip thickness below 2.0 mm. In such applications, it can be unnecessary to thin down the stack.
Where thinning of the contact probe tip wafer 212 is desired, preferably, thinning is performed prior to bonding of the contact probe tip wafer 212 with the plate wafer 140. A contact probe tip wafer 210 having undergone thinning by way of mechanical polishing, CMP polishing, and/or etch processing can have a thickness generally in a range of from 100-500 μm range. The contact probe tip wafer 210 provides a mounting surface during processing to thin the cap wafer 132, and during sawing steps; therefore, the contact probe tip wafer 210 should have a thickness sufficient to endure further processing. Thus, a thicker contact probe tip wafer 210 provides better stress relief to a wafer stack during wafer-level processing steps and to the micro mover structure after dicing.
Where thinning of the cap wafer 132 is desired, thinning can be preferably be performed subsequent to thinning of the contact probe tip wafer 210, as shown in
Cuts through the cap wafer 132 should be formed to remove portions of the cap wafer 132 and provide access to the bond pads 180 formed on the stationary portion 120, and further to separate the wafer stack into die. Preferably, at least a portion of dicing grooves 196 of the cap wafer 132 is exposed during thinning of the cap wafer and the exposed pattern can assist in determining a correct position of the cuts at this step. After or while the bond pads 180 are exposed, dicing is performed. There are different options for depth of the cut at the dicing step. Preferably, both pad expose and dicing are done using sawing. The micro-mover after pad-expose cuts and dicing is shown in
When the stage stack 100 is assembled and, if necessary, thinned, at least one permanent magnet can generally be aligned with the coils 102 and a ferromagnetic shell enclosing the die. The combination of at least one permanent magnet and a ferromagnetic shell creates a required distribution of magnetic field in the gap between them, where the die is located and, therefore, enables electromagnetic actuation. For example, the permanent magnet can be located under the tip wafer 212 and the ferromagnetic shell can include a steel plate located above the top cap 130. In other embodiments, some other metals or alloys can be employed.
In contrast with a micro mover having one cap, the micro mover structure with two caps provides much better protection of the movable plate and does not require mounting on a temporary carrier. In the example given above, the contact probe tip wafer can be considered a substitute for a cap, while providing mechanical and environmental protection during processing as would a cap. However, a temporary carrier can be employed to increase mechanical strength of the stack and decrease yield loss due to handling and processing of thinned stacks of wafers.
The foregoing description of the present invention have been presented for purposes of illustration and description. It is not intended to be exhaustive or to limit the invention to the precise forms disclosed. Many modifications and variations will be apparent to practitioners skilled in this art. The embodiments were chosen and described in order to best explain the principles of the invention and its practical application, thereby enabling others skilled in the art to understand the invention for various embodiments and with various modifications as are suited to the particular use contemplated. It is intended that the scope of the invention be defined by the following claims and their equivalents.
This application claims benefit to the following U.S. Provisional Application: U.S. Provisional Patent Application No. 60/813,817 entitled BONDED CHIP ASSEMBLY WITH A MICRO-MOVER FOR MICROELECTROMECHANICAL SYSTEMS, by Nickolai Belov et al., filed Jun. 15, 2006, Attorney Docket No. NANO-01041US0. This application incorporates by reference all of the following co-pending applications and the following issued patents: U.S. patent application Ser. No. 11/177,550, entitled “Media for Writing Highly Resolved Domains,” by Yevgeny Vasilievich Anoikin, filed Jul. 8, 2005, Attorney Docket No. NANO-01032US1; U.S. patent application Ser. No. 11/177,639, entitled “Patterned Media for a High Density Data Storage Device,” by Zhaohui Fan et al., filed Jul. 8, 2005, Attorney Docket No. NANO-01033US0; U.S. patent application Ser. No. 11/177,062, entitled “Method for Forming Patterned Media for a High Density Data Storage Device,” by Zhaohui Fan et al, filed by Jul. 8, 2005, Attorney Docket No. NANO-01033US1; U.S. patent application Ser. No. 11/177,599, entitled “High Density Data Storage Devices with Read/Write Probes with Hollow or Reinforced Tips,” by Nickolai Belov, filed Jul. 8, 2005, Attorney Docket No. NANO-01034US0; U.S. patent application Ser. No. 11/177,731, entitled “Methods for Forming High Density Data Storage Devices with Read/Write Probes with Hollow or Reinforced Tips,” by Nickolai Belov, filed Jul. 8, 2005, Attorney Docket No. NANO-01034US1; U.S. patent application Ser. No. 11/177,642, entitled “High Density Data Storage Devices with Polarity-Dependent Memory Switching Media,” by Donald E. Adams, et al., filed Jul. 8, 2005, Attorney Docket No. NANO-01035US0; U.S. patent application Ser. No. 11/178,060, entitled “Methods for Writing and Reading in a Polarity-Dependent Memory Switching Media,” by Donald E. Adams, et al., filed Jul. 8, 2005, Attorney Docket No. NANO-01035US1; U.S. patent application Ser. No. 11/178,061, entitled “High Density Data Storage Devices with a Lubricant Layer Comprised of a Field of Polymer Chains,” by Yevgeny Vasilievich Anoikin, filed Jul. 8, 2005, Attorney Docket No. NANO-01036US0; U.S. patent application Ser. No. 11/004,153, entitled “Methods for Writing and Reading Highly Resolved Domains for High Density Data Storage,” by Thomas F. Rust et al., filed Dec. 3, 2004, Attorney Docket No. NANO-01024US1; U.S. patent application Ser. No. 11/003,953, entitled “Systems for Writing and Reading Highly Resolved Domains for High Density Data Storage,” by Thomas F. Rust et al., filed Dec. 3, 2004, Attorney Docket No. NANO-01024US2; U.S. patent application Ser. No. 11/004,709, entitled “Methods for Erasing Bit Cells in a High Density Data Storage Device,” by Thomas F. Rust et al., filed Dec. 3, 2004, Attorney Docket No. NANO-01031US0; U.S. patent application Ser. No. 11/003,541, entitled “High Density Data Storage Device Having Erasable Bit Cells,” by Thomas F. Rust et al, filed Dec. 3, 2004, Attorney Docket No. NANO-01031US1; U.S. patent application Ser. No. 11/003,955, entitled “Methods for Erasing Bit Cells in a High Density Data Storage Device,” by Thomas F. Rust et al., filed Dec. 3, 2004, Attorney Docket No. NANO-01031US2; U.S. patent application Ser. No. 10/684,760, entitled “Fault Tolerant Micro-Electro Mechanical Actuators,” by Thomas F. Rust, filed Oct. 14, 2003, Attorney Docket No. NANO-01015US1; U.S. patent application Ser. No. 10/685,045, entitled “Phase Change Media for High Density Data Storage,” by Thomas F. Rust, filed Oct. 14, 2003, Attorney Docket No. NANO-01019US1; U.S. patent application Ser. No. 09/465,592, entitled “Molecular Memory Medium and Molecular Memory Integrated Circuit,” by Joanne P. Culver, et al., filed Dec. 17, 1999, Attorney Docket No. NANO-01000US0; U.S. Pat. No. 5,453,970, entitled “Molecular Memory Medium and Molecular Memory Disk Drive for Storing Information Using a Tunnelling Probe,” issued Sep. 26, 1995 to Thomas F. Rust, et al.; U.S. Pat. No. 6,982,898, entitled “Molecular Memory Integrated Circuit Utilizing Non-Vibrating Cantilevers,” Attorney Docket No. NANO-01011US1, issued Jan. 3, 2006 to Thomas F. Rust, et al.,; U.S. Pat. No. 6,985,377, entitled “Phase Change Media for High Density Data Storage,” Attorney Docket No. NANO-01019US1, issued Jan. 10, 2006 to Thomas F. Rust, et al.
Number | Date | Country | |
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60813817 | Jun 2006 | US |