US20080303383A1 - Shock resistant and mode mixing resistant torsional hinged device - Google Patents
Shock resistant and mode mixing resistant torsional hinged device Download PDFInfo
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- US20080303383A1 US20080303383A1 US11/758,411 US75841107A US2008303383A1 US 20080303383 A1 US20080303383 A1 US 20080303383A1 US 75841107 A US75841107 A US 75841107A US 2008303383 A1 US2008303383 A1 US 2008303383A1
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- 230000035939 shock Effects 0.000 title claims abstract description 19
- 238000000034 method Methods 0.000 claims description 10
- 230000001154 acute effect Effects 0.000 claims 4
- 230000008901 benefit Effects 0.000 description 6
- 230000000694 effects Effects 0.000 description 5
- 230000010355 oscillation Effects 0.000 description 4
- 230000009471 action Effects 0.000 description 3
- 230000003247 decreasing effect Effects 0.000 description 2
- 230000008569 process Effects 0.000 description 2
- 238000005086 pumping Methods 0.000 description 2
- 230000004075 alteration Effects 0.000 description 1
- 230000000712 assembly Effects 0.000 description 1
- 238000000429 assembly Methods 0.000 description 1
- 239000011449 brick Substances 0.000 description 1
- 238000010276 construction Methods 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 230000009467 reduction Effects 0.000 description 1
- 238000006467 substitution reaction Methods 0.000 description 1
- 239000000758 substrate Substances 0.000 description 1
- 208000005123 swayback Diseases 0.000 description 1
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Classifications
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- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B26/00—Optical devices or arrangements for the control of light using movable or deformable optical elements
- G02B26/08—Optical devices or arrangements for the control of light using movable or deformable optical elements for controlling the direction of light
- G02B26/0816—Optical devices or arrangements for the control of light using movable or deformable optical elements for controlling the direction of light by means of one or more reflecting elements
- G02B26/0833—Optical devices or arrangements for the control of light using movable or deformable optical elements for controlling the direction of light by means of one or more reflecting elements the reflecting element being a micromechanical device, e.g. a MEMS mirror, DMD
- G02B26/0858—Optical devices or arrangements for the control of light using movable or deformable optical elements for controlling the direction of light by means of one or more reflecting elements the reflecting element being a micromechanical device, e.g. a MEMS mirror, DMD the reflecting means being moved or deformed by piezoelectric means
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- B—PERFORMING OPERATIONS; TRANSPORTING
- B81—MICROSTRUCTURAL TECHNOLOGY
- B81B—MICROSTRUCTURAL DEVICES OR SYSTEMS, e.g. MICROMECHANICAL DEVICES
- B81B3/00—Devices comprising flexible or deformable elements, e.g. comprising elastic tongues or membranes
- B81B3/0064—Constitution or structural means for improving or controlling the physical properties of a device
- B81B3/0067—Mechanical properties
- B81B3/0078—Constitution or structural means for improving mechanical properties not provided for in B81B3/007 - B81B3/0075
-
- B—PERFORMING OPERATIONS; TRANSPORTING
- B81—MICROSTRUCTURAL TECHNOLOGY
- B81B—MICROSTRUCTURAL DEVICES OR SYSTEMS, e.g. MICROMECHANICAL DEVICES
- B81B7/00—Microstructural systems; Auxiliary parts of microstructural devices or systems
- B81B7/0009—Structural features, others than packages, for protecting a device against environmental influences
- B81B7/0012—Protection against reverse engineering, unauthorised use, use in unintended manner, wrong insertion or pin assignment
-
- B—PERFORMING OPERATIONS; TRANSPORTING
- B81—MICROSTRUCTURAL TECHNOLOGY
- B81B—MICROSTRUCTURAL DEVICES OR SYSTEMS, e.g. MICROMECHANICAL DEVICES
- B81B2201/00—Specific applications of microelectromechanical systems
- B81B2201/04—Optical MEMS
- B81B2201/042—Micromirrors, not used as optical switches
-
- B—PERFORMING OPERATIONS; TRANSPORTING
- B81—MICROSTRUCTURAL TECHNOLOGY
- B81B—MICROSTRUCTURAL DEVICES OR SYSTEMS, e.g. MICROMECHANICAL DEVICES
- B81B2203/00—Basic microelectromechanical structures
- B81B2203/01—Suspended structures, i.e. structures allowing a movement
- B81B2203/0109—Bridges
Definitions
- the present invention relates generally to the field of torsional hinged Micro Electro Mechanical Systems (MEMS) oscillating devices. More particularly, the invention relates to a shock resistant and mode mixing resistant actuator structure for driving the torsional hinged device oscillations at a resonant frequency.
- MEMS Micro Electro Mechanical Systems
- the assembly is comprised of first and second elongated members such as at least one torsional hinge for supporting an oscillating functional member such as a MEMS mirror along a pivot axis.
- Each of the elongated members extends from an oscillating functional member to an end portion.
- the end portion of the at least one torsional hinge is supported and attached to a pair of piezoelectric elements that extend between the end portion of the torsional hinge and a support base.
- Each piezoelectric element is typically a long thin parallelepiped or brick shaped structure having a thickness dimension, a width dimension, and a length or height dimension, and each piezoelectric element of the pair of elements is mounted on end to a support base such that the length or height dimension extends perpendicularly and away from the support base and so that the width dimension of one of the piezoelectric elements is not parallel to the width dimension of the other one of the pair of piezoelectric elements.
- Mounting piezoelectric elements so that the width dimension forms a 15 degree angle with a line perpendicular to the pivot axis of the oscillation device has been found to be particularly effective.
- FIGS. 1A-1B are a perspective view and an end view, respectively, of a piezoelectric driven resistant oscillating device that is susceptible to both mechanical shock and mode mixing;
- FIGS. 1C-1D show perspective views of alternative embodiments with only one torsional hinge
- FIGS. 2A-2B are a top view and a side view, respectively, of the device of FIG. 1A illustrating the effects of mechanical shock in the X, Y and Z directions on the oscillating device;
- FIGS. 3A-3B are an end view and a side view, respectively, of the device of FIG. 1A illustrating cross-modal effects on the oscillating device;
- FIGS. 4A-4B are a perspective view and a top view respectively of a piezoelectric driven torsional hinged oscillating device incorporating the present invention.
- the device 10 comprises first and second elongated members 14 a and 14 b that are attached to and extend from the oscillating device or mirror 12 to end portions 16 a and 16 b, respectively. At least one, and preferably both, of the elongated members 14 a and 14 b comprise torsional hinges.
- the end portions 16 a and 16 b are in turn supported by structures 18 a and 18 b, respectively, which extend between the base support 20 and the end portions 16 a and 16 b of the resonant mirror.
- At least one of the structures 18 a and 18 b comprise a pair of piezoelectric devices or towers such as elements 22 a and 24 a that comprise structure 18 a.
- both structures 18 a and 18 b comprise a pair of piezoelectric elements.
- structure 18 b may simply comprise a non-piezoelectric mechanical support members, or could comprise a pair of piezoelectric elements that are not electrically connected as shown in FIG. 1C .
- both elongated members 14 a and 14 b are torsional hinges.
- end portion 16 b of elongated member 14 b simply be supported by a receiving aperture 26 as shown in FIG. 1D and not provide torsional action to the device 10 .
- a receiving aperture 26 as shown in FIG. 1D
- the remaining discussion will be with respect to an oscillating device that comprises two pairs of piezoelectric elements and two torsional hinges.
- the typical piezoelectric elements or towers are a thin elongated parallelepiped having a first end 28 mounted or soldered to a substrate or base support 20 and a second end 30 attached to the end portions of 16 a and 16 b of the torsional hinges 14 a and 14 b.
- Each of the piezoelectric elements have a thickness dimension “T,” a width dimension “W” and a length or height dimension “L.”
- the piezoelectric elements are arranged side by side in pairs with the large faces (W dimension) of each pair facing each other.
- a pair of piezoelectric elements or towers are electrically connected so that each one of the pair operates 180 degrees out of phase with the other to create an up and down pumping action as indicated by the large directional arrows 32 a and 32 b.
- This pumping action in turn causes the oscillating mirror 12 or other functional device to oscillate at its resonant frequency around pivot axis 33 .
- two pairs of piezoelectric elements or towers such structures 18 a and 18 b are used, elements opposite each other and attached to the end portion of different torsional hinges operate in phase.
- FIGS. 2A and 2B the effect of mechanical shock received along axes X, Y and Z of the device of FIG. 1A will be discussed. Parts of the device in FIGS. 2A and 2B that are common with the device of FIG. 1A will carry the same reference numbers. As will be appreciated, there is significant resistance to mechanical shock along the Y and Z axes and, for most situations therefore, shock along the Y and Z axes is not a concern. However, because the piezoelectric elements 22 a, 22 b, 24 a, and 24 b are very thin, mechanical shock along the X axis can snap or break the piezoelectric elements at end 28 where they are attached to the base support 20 .
- the piezoelectric element of a pair of elements or towers extends and contracts out of phase as shown by arrows 32 a and 32 b, which causes the oscillating device or mirror to oscillate or rotate at the same or resonant frequency around pivot axis 33 as the piezoelectric elements contract and extend.
- various packages and assembly processes add imbalances to the operation of the device which in turn causes other modes of the assembly to be excited. This may result in one or more other resonant modes, such as indicated by arrow 38 , to be mixed with the intended rotational mode indicated by arcuate arrow 40 . Since such mixing of the mode causes noise, loss of rotation and out of phase oscillations, a means for reducing mode mixing is also desirable.
- each element of the pair of piezoelectric elements or towers is located directly opposite the other. This arrangement allows the piezoelectric elements or towers to sway back and forth. The swaying may be together or out of phase with each other.
- FIGS. 4A and 4B there is illustrated an arrangement of the piezoelectric elements or towers that stiffens the assembly against swaying, which in turn increases the resistance to both shock and mode mixing.
- the two elements of each pair of piezoelectric elements or towers are arranged to form a chevron shape. That is, the width dimension W of piezoelectric elements 22 a and 22 b are not aligned with each other and are not parallel to each other.
- a preferred arrangement has been found in locating a pair of the piezoelectric elements so that each one in the pair is at a 15 degree angle with a line 42 perpendicular to the pivot axis 33 and lying in the same plane as the pivot axis 33 .
- the resistance against swaying is decreased as the angle is decreased and that the most dramatic reduction of the swaying is at very low angles.
- an angle of 15 degrees has been found to be particularly useful, almost any angle 44 above zero provides improved resistance.
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- Mechanical Engineering (AREA)
- Computer Hardware Design (AREA)
- Microelectronics & Electronic Packaging (AREA)
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Health & Medical Sciences (AREA)
- General Health & Medical Sciences (AREA)
- Toxicology (AREA)
- Mechanical Optical Scanning Systems (AREA)
- Mechanical Light Control Or Optical Switches (AREA)
Abstract
Description
- The present invention relates generally to the field of torsional hinged Micro Electro Mechanical Systems (MEMS) oscillating devices. More particularly, the invention relates to a shock resistant and mode mixing resistant actuator structure for driving the torsional hinged device oscillations at a resonant frequency.
- The use of rotating polygon scanning mirrors in laser printers to provide a beam sweep or scan of the image of a modulated light source across a photoresisted medium, such as a rotating drum, is well known. More recently, there have been efforts to use a much less expensive flat member with a single reflective surface, such as a MEMS resonant oscillating mirror, to provide the scanning beam. Other devices using resonant oscillating members, other than mirrors, may also benefit from this invention. These torsional hinged resonant scanning devices provide excellent performance at a very advantageous cost. Several techniques are available for driving the torsional hinged resonant scanning device, but the use of piezoelectric elements has been found to be both effective and inexpensive. However, as is the case with almost every technology using piezoelectric driving elements has its own set of problems. More specifically, the long thin piezoelectric elements used to excite the rotational scanning of resonant devices such as mirror assemblies are susceptible to mode mixing and mechanical shock.
- Therefore, rugged methods and structures that facilitate the use of piezoelectric driving elements without a corresponding increase in complexity or cost would be advantageous.
- These problems of mode mixing and mechanical shock are generally solved or circumvented, and technical advantages are generally achieved, by the embodiments of the present invention which provide a shock resistant and mode mixing resistant assembly using piezoelectric elements to provide resonant oscillations to a torsional hinged device. The assembly is comprised of first and second elongated members such as at least one torsional hinge for supporting an oscillating functional member such as a MEMS mirror along a pivot axis. Each of the elongated members (including at least one torsional hinge) extends from an oscillating functional member to an end portion. The end portion of the at least one torsional hinge is supported and attached to a pair of piezoelectric elements that extend between the end portion of the torsional hinge and a support base. Each piezoelectric element is typically a long thin parallelepiped or brick shaped structure having a thickness dimension, a width dimension, and a length or height dimension, and each piezoelectric element of the pair of elements is mounted on end to a support base such that the length or height dimension extends perpendicularly and away from the support base and so that the width dimension of one of the piezoelectric elements is not parallel to the width dimension of the other one of the pair of piezoelectric elements. Mounting piezoelectric elements so that the width dimension forms a 15 degree angle with a line perpendicular to the pivot axis of the oscillation device has been found to be particularly effective.
- The foregoing has broadly outlined the features of the present invention in order that the detailed description of the invention that follows may be better understood. Additional features and advantages will be described hereinafter, which form the subject of the claims of the invention. It should be appreciated by those skilled in the art that the conception and specific embodiments disclosed may be readily utilized as a basis for modifying or designing other structures or processes for carrying out the same purpose of the present invention. It should also be realized by those skilled in the art that such constructions do not depart from the spirit or scope of the invention as set forth in the appended claims.
- For a more complete understanding of the present invention, and the advantages thereof, reference is made to the following descriptions taken in conjunction with the accompanying drawings, in which:
-
FIGS. 1A-1B are a perspective view and an end view, respectively, of a piezoelectric driven resistant oscillating device that is susceptible to both mechanical shock and mode mixing; -
FIGS. 1C-1D show perspective views of alternative embodiments with only one torsional hinge; -
FIGS. 2A-2B are a top view and a side view, respectively, of the device ofFIG. 1A illustrating the effects of mechanical shock in the X, Y and Z directions on the oscillating device; -
FIGS. 3A-3B are an end view and a side view, respectively, of the device ofFIG. 1A illustrating cross-modal effects on the oscillating device; and -
FIGS. 4A-4B are a perspective view and a top view respectively of a piezoelectric driven torsional hinged oscillating device incorporating the present invention. - The making and using of the described embodiments are discussed in detail below. It should be appreciated, however, that the present invention provides many applicable inventive concepts that can be embodied in a wide variety of specific contexts. The specific embodiments discussed are illustrative of specific ways to make and use the invention, and should not limit the scope of the invention.
- Referring now to
FIGS. 1A and 1B there is illustrated a piezoelectric driven torsional hingeddevice 10, such as amirror 12 that is not resistant to mechanical shock or cross-modal effects. As shown, thedevice 10 comprises first and second elongated members 14 a and 14 b that are attached to and extend from the oscillating device ormirror 12 to end portions 16 a and 16 b, respectively. At least one, and preferably both, of the elongated members 14 a and 14 b comprise torsional hinges. The end portions 16 a and 16 b are in turn supported by structures 18 a and 18 b, respectively, which extend between thebase support 20 and the end portions 16 a and 16 b of the resonant mirror. At least one of the structures 18 a and 18 b, and preferably both, comprise a pair of piezoelectric devices or towers such as elements 22 a and 24 a that comprise structure 18 a. Although, as mentioned above, it is preferable that both structures 18 a and 18 b comprise a pair of piezoelectric elements. However, structure 18 b may simply comprise a non-piezoelectric mechanical support members, or could comprise a pair of piezoelectric elements that are not electrically connected as shown inFIG. 1C . Also as was mentioned above, it is preferred that both elongated members 14 a and 14 b are torsional hinges. However, it is possible that the end portion 16 b of elongated member 14 b simply be supported by a receivingaperture 26 as shown inFIG. 1D and not provide torsional action to thedevice 10. Although these alternate embodiments may also benefit from the teaching of the present invention, the remaining discussion will be with respect to an oscillating device that comprises two pairs of piezoelectric elements and two torsional hinges. - Referring again to
FIGS. 1A and 1B , it is seen that the typical piezoelectric elements or towers are a thin elongated parallelepiped having afirst end 28 mounted or soldered to a substrate orbase support 20 and asecond end 30 attached to the end portions of 16 a and 16 b of the torsional hinges 14 a and 14 b. Each of the piezoelectric elements have a thickness dimension “T,” a width dimension “W” and a length or height dimension “L.” The piezoelectric elements are arranged side by side in pairs with the large faces (W dimension) of each pair facing each other. A pair of piezoelectric elements or towers are electrically connected so that each one of the pair operates 180 degrees out of phase with the other to create an up and down pumping action as indicated by the large directional arrows 32 a and 32 b. This pumping action in turn causes the oscillatingmirror 12 or other functional device to oscillate at its resonant frequency aroundpivot axis 33. It should also be noted that when two pairs of piezoelectric elements or towers, such structures 18 a and 18 b are used, elements opposite each other and attached to the end portion of different torsional hinges operate in phase. - Referring to
FIGS. 2A and 2B , the effect of mechanical shock received along axes X, Y and Z of the device ofFIG. 1A will be discussed. Parts of the device inFIGS. 2A and 2B that are common with the device ofFIG. 1A will carry the same reference numbers. As will be appreciated, there is significant resistance to mechanical shock along the Y and Z axes and, for most situations therefore, shock along the Y and Z axes is not a concern. However, because the piezoelectric elements 22 a, 22 b, 24 a, and 24 b are very thin, mechanical shock along the X axis can snap or break the piezoelectric elements atend 28 where they are attached to thebase support 20. Large double headedarrow 34 and dotted lines 36 a, 36 b, 36c, and 36d illustrate the direction of a shock event along the X axis and the resulting deflection of the piezoelectric elements respectively. An arrangement that can resist mechanical shock in the X direction would be very advantageous. - Referring to
FIG. 3A , cross-modal effects are discussed. As was discussed above, the piezoelectric element of a pair of elements or towers extends and contracts out of phase as shown by arrows 32 a and 32 b, which causes the oscillating device or mirror to oscillate or rotate at the same or resonant frequency aroundpivot axis 33 as the piezoelectric elements contract and extend. Unfortunately, various packages and assembly processes add imbalances to the operation of the device which in turn causes other modes of the assembly to be excited. This may result in one or more other resonant modes, such as indicated byarrow 38, to be mixed with the intended rotational mode indicated byarcuate arrow 40. Since such mixing of the mode causes noise, loss of rotation and out of phase oscillations, a means for reducing mode mixing is also desirable. - It has been discovered that one source of these problems is that each element of the pair of piezoelectric elements or towers is located directly opposite the other. This arrangement allows the piezoelectric elements or towers to sway back and forth. The swaying may be together or out of phase with each other.
- Therefore, referring now to
FIGS. 4A and 4B , there is illustrated an arrangement of the piezoelectric elements or towers that stiffens the assembly against swaying, which in turn increases the resistance to both shock and mode mixing. As shown, the two elements of each pair of piezoelectric elements or towers are arranged to form a chevron shape. That is, the width dimension W of piezoelectric elements 22 a and 22 b are not aligned with each other and are not parallel to each other. A preferred arrangement has been found in locating a pair of the piezoelectric elements so that each one in the pair is at a 15 degree angle with aline 42 perpendicular to thepivot axis 33 and lying in the same plane as thepivot axis 33. It is also noted that the resistance against swaying is decreased as the angle is decreased and that the most dramatic reduction of the swaying is at very low angles. Thus, although an angle of 15 degrees has been found to be particularly useful, almost anyangle 44 above zero provides improved resistance. - Although the present invention and its advantages have been described in detail, it should be understood that various changes, substitutions, and alterations can be made herein without departing from the spirit and scope of the invention as defined by the appended claims.
- Moreover, the scope of the present application is not intended to be limited to the particular embodiments of the structure, methods, and steps described in the specification. As one of ordinary skill in the art will readily appreciate from the disclosure of the present invention, such structures, methods, and steps presently existing or later to be developed, that perform substantially the same function or achieve substantially the same result as the corresponding embodiments described herein may be utilized according to the present invention. Accordingly, the appended claims are intended to include within their scope such structure, methods, and steps.
Claims (13)
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| US11/758,411 US7471032B1 (en) | 2007-06-05 | 2007-06-05 | Shock resistant and mode mixing resistant torsional hinged device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| US11/758,411 US7471032B1 (en) | 2007-06-05 | 2007-06-05 | Shock resistant and mode mixing resistant torsional hinged device |
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| Publication Number | Publication Date |
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| US20080303383A1 true US20080303383A1 (en) | 2008-12-11 |
| US7471032B1 US7471032B1 (en) | 2008-12-30 |
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Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US20100277251A1 (en) * | 2009-05-01 | 2010-11-04 | Seiko Epson Corporation | Oscillator, oscillator array and an electronic apparatus |
| WO2020129430A1 (en) * | 2018-12-19 | 2020-06-25 | Ricoh Company, Ltd. | Movable device, distance measurement device, image projection apparatus, vehicle, and mount |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US9933249B2 (en) | 2013-12-16 | 2018-04-03 | Waters Technologies Corporation | Dynamic mechanical analyzer and sample fixtures for a dynamic mechanical analyzer |
Citations (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US6803938B2 (en) * | 2002-05-07 | 2004-10-12 | Texas Instruments Incorporated | Dynamic laser printer scanning alignment using a torsional hinge mirror |
| US20050078169A1 (en) * | 2003-10-08 | 2005-04-14 | Tumer Arthur Monroe | Apparatus and methods for adjusting the rotational frequency of a scanning device |
-
2007
- 2007-06-05 US US11/758,411 patent/US7471032B1/en active Active
Patent Citations (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US6803938B2 (en) * | 2002-05-07 | 2004-10-12 | Texas Instruments Incorporated | Dynamic laser printer scanning alignment using a torsional hinge mirror |
| US20050078169A1 (en) * | 2003-10-08 | 2005-04-14 | Tumer Arthur Monroe | Apparatus and methods for adjusting the rotational frequency of a scanning device |
Cited By (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US20100277251A1 (en) * | 2009-05-01 | 2010-11-04 | Seiko Epson Corporation | Oscillator, oscillator array and an electronic apparatus |
| US8247948B2 (en) * | 2009-05-01 | 2012-08-21 | Seiko Epson Corporation | Oscillator, oscillator array and an electronic apparatus |
| WO2020129430A1 (en) * | 2018-12-19 | 2020-06-25 | Ricoh Company, Ltd. | Movable device, distance measurement device, image projection apparatus, vehicle, and mount |
| CN113196133A (en) * | 2018-12-19 | 2021-07-30 | 株式会社理光 | Movable device, distance measuring device, image projection device, vehicle, and pedestal |
| US12091309B2 (en) | 2018-12-19 | 2024-09-17 | Ricoh Company, Ltd. | Movable device, distance measurement device, image projection apparatus, vehicle, and mount |
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| Publication number | Publication date |
|---|---|
| US7471032B1 (en) | 2008-12-30 |
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