WO2004061389A1 - Laser digitizer system for dental applications - Google Patents

Laser digitizer system for dental applications Download PDF

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Publication number
WO2004061389A1
WO2004061389A1 PCT/US2003/041701 US0341701W WO2004061389A1 WO 2004061389 A1 WO2004061389 A1 WO 2004061389A1 US 0341701 W US0341701 W US 0341701W WO 2004061389 A1 WO2004061389 A1 WO 2004061389A1
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WO
WIPO (PCT)
Prior art keywords
image
laser
light
scanner
laser digitizer
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Ceased
Application number
PCT/US2003/041701
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English (en)
French (fr)
Inventor
Henley Quadling
Mark Quadling
Alan Blair
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
D3D LP
Original Assignee
D3D LP
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by D3D LP filed Critical D3D LP
Priority to JP2004564915A priority Critical patent/JP2006514739A/ja
Priority to DE60326881T priority patent/DE60326881D1/de
Priority to DK03800393T priority patent/DK1579171T3/da
Priority to CA002511828A priority patent/CA2511828C/en
Priority to EP03800393A priority patent/EP1579171B1/en
Priority to AU2003300135A priority patent/AU2003300135B2/en
Publication of WO2004061389A1 publication Critical patent/WO2004061389A1/en
Anticipated expiration legal-status Critical
Ceased legal-status Critical Current

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Classifications

    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01B—MEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
    • G01B11/00—Measuring arrangements characterised by the use of optical techniques
    • G01B11/24—Measuring arrangements characterised by the use of optical techniques for measuring contours or curvatures
    • G01B11/25—Measuring arrangements characterised by the use of optical techniques for measuring contours or curvatures by projecting a pattern, e.g. one or more lines, moiré fringes on the object
    • G01B11/2518—Projection by scanning of the object
    • A—HUMAN NECESSITIES
    • A61—MEDICAL OR VETERINARY SCIENCE; HYGIENE
    • A61C—DENTISTRY; APPARATUS OR METHODS FOR ORAL OR DENTAL HYGIENE
    • A61C9/00—Impression cups, i.e. impression trays; Impression methods
    • A61C9/004—Means or methods for taking digitized impressions
    • A61C9/0046—Data acquisition means or methods
    • A61C9/0053—Optical means or methods, e.g. scanning the teeth by a laser or light beam
    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01B—MEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
    • G01B11/00—Measuring arrangements characterised by the use of optical techniques
    • G01B11/24—Measuring arrangements characterised by the use of optical techniques for measuring contours or curvatures

Definitions

  • the invention relates to three-dimensional imaging of physical objects.
  • the invention relates to laser imaging of dental items including molds, castings, dentition, prepared dentition and the like.
  • the 3D image may be generated by a computer that processes data representing the surfaces and contours of a physical object.
  • the computer displays the 3D image on a screen or a computer monitor.
  • the data may be generated by optically scanning the physical object and detecting or capturing the light reflected off of the object. Based on processing techniques such as Moire, interferometry, and laser triangulation the shape, surfaces and/or contours of the object may be modeled by the computer.
  • the Moire technique uses a structured white light to project a 2D image on the object to be imaged.
  • the Moire technique uses a pattern that has a sinusoidal intensity pattern.
  • the projected image intensity pattern observed from a position other than the projected angle does not appear sinusoidal. Therefore, an inferred point-by-point phase angle between an observed and a projected image may be correlated to the height data Z at each observed pixel point.
  • Interferometry methods may then use a reference beam and a scanning beam to infer 3D information based on an optical interference between the two beams.
  • Laser triangulation methods project a laser dot or beam onto an object from a known direction. The laser beam is scanned across the surface of the object following an arc.
  • the laser beam is imaged by an imaging system from a different known direction.
  • the known baseline and angle between the projector and imaging system provides sufficient information to deduce the 3D location of the reflected dot from the surface of the object being scanned, utilizing known triangulation techniques.
  • Such scanning may also result in an inaccurate reading of depth of field and uniformity of a line width due to the scanned arc.
  • Systems have been developed using special optics that increase the depth measurement and resolution. However, some special optics adversely effect and distort the optical image and limit the speed at which the system may acquire sufficient data to generate a 3D image.
  • Laser triangulation methods also may scan one or more laser lines across an object.
  • the laser lines may be generated through a diffractive lens.
  • the intensity of the laser line(s) may vary along the length of the projected line(s), resulting in inaccurate measurements and imaging of the object.
  • the laser line systems are also susceptible to laser speckle, which may appear as a mottled pattern of randomly distributed "blobs of light.”
  • Laser speckle may be caused by an interference at the image plane of coherent light reflected by a rough surface.
  • the mottled pattern may introduce noise and uncertainty into the measurement, due to a difficulty in distinguishing between useful intensity data, and speckle intensity data.
  • the embodiments provide a laser imaging system that generates a three- dimensional image of a scanned physical object such as a dental item.
  • An embodiment includes laser imaging systems, methods, apparatuses, and techniques that provide laser digitization of a physical object to obtain a visual image of the object.
  • the visual image may be displayed on a computer monitor, screen, display, or the like.
  • a laser digitizer may include a light source, a scanner, a flat-field lens, an image capture instrument, and a processor configured to carry out instructions based on code, and process digital data.
  • the laser digitizer may also include an object positioning system for positioning an object within a field of view of the scanner and the image capture instrument.
  • the light source may include a laser LED and collimating optics configured to produce a coUimated beam of light.
  • the collimated beam of light is projected to the scanner.
  • the scanner redirects or scans the collimated beam of light so that the beam is scanned through at least two axes.
  • the scanned beam is projected toward the lens, which focuses the beam as a dot on the surface of the object.
  • the lens focuses the dot ⁇ on the object so that the dot traverses a curvilinear segment across the object.
  • the image capture instrument detects the light reflected from the object and generates data representing a captured image of the scanned beam.
  • the image capture system may be configured to capture images of one or more scanned curvilinear segments during an exposure period.
  • the computer processes the data to generate the three-dimensional visual image of the object on a computer monitor, a screen, or other display. Multiple images of the object may be recorded and processed by the computer to produce a three-dimensional map of the object. The multiple images can be captured from multiple positions and orientations of the object. The individual images are merged to create an overall three-dimensional ("3D") map of the object.
  • 3D three-dimensional
  • Figure 1 illustrates an example of a prior art laser line system.
  • Figure 2a illustrates a top view of a laser digitizer system for dental applications.
  • Figure 2b illustrates a front view of a laser digitizer system for dental applications.
  • Figure 3 illustrates an image of a light pattern of a laser digitizer of Figures
  • Figure 4 illustrates the light pattern of Figure 3 as projected on an object to be imaged.
  • Figure 5 illustrates a reflection of the light pattern of Figure 3 as detected by image capture instrument.
  • Figure 6 illustrates an embodiment of an object positioner of the laser digitizer system of Figures 2a and 2b.
  • FIG 1 illustrates an example of a prior art laser line imaging system 100.
  • the prior art laser line imaging system 100 has a transmitter 102 and a receiver 108.
  • the transmitter 102 includes a laser light source 104 and transmission optics 106.
  • the transmitter 102 projects a planar laser light on an object 120 within a field of view of the transmitter 102.
  • the planar laser light incident on the object forms a straight line on the object 120.
  • the projected laser line is produced by either a cylindrical lens or diffractive optical element 106.
  • the light reflected from the object 120 is detected by the camera 108.
  • the camera 108 has an optical axis at a known angle to the transmitter 102.
  • the light is picked up by an optical lens 112 which focuses the reflected light onto a matrix of photo-detectors 110.
  • the contour of the object 120 having differences in the elevation can be imaged based on the image projected on the matrix of photo- detectors 110.
  • FIGS 2a and 2b illustrate an example of a laser digitizer system 200 configured to generate a 3D image of a dental item.
  • the laser digitizer system 200 includes a laser light source 202, an optical scanner 222, a flat-field lens 228, that may be known as an F-Theta lens, an image capture instrument 230, and a processor 236.
  • the laser digitizer system 200 may also include a positioner (not shown) for securing and positioning an object to be imaged.
  • the laser digitizer system 200 may also include a variable beam expander 242 optically positioned between the laser source and the scanner 222.
  • the laser light source 202 generates a laser beam that is projected and scanned across an object to be imaged by the scanner 222 and the F-Theta lens 228.
  • the scanned light is reflected from the object 220 and detected by the image capture instrument 230, which generates a signal representative of the detected light.
  • the laser light source 202 may include collimating optics (not shown) that produce a collimated light beam 238 having parallel rays of laser light. This collimated light beam 238 is projected towards a two-axis optical scanner 222.
  • the laser light source 202 may include a laser diode or LED configured to generate a laser light beam that may have an elliptical-shaped beam.
  • the collimating optics may be configured to circularize the elliptical beam and to generate a circular spot.
  • the circular spot may be used to scan a uniform line across the surface of the object 220.
  • the laser diode may be any commercially available laser diode configured to emit a laser light beam, such as a 10 mW laser diode from Blue Sky Research having a 4 mm beam size at a 635 nm wavelength (part number MINI-0635-101C40W).
  • the laser light source 202 also may be configured to modulate laser light.
  • the laser light source 202 also may be coupled to a modulator that adjusts or interrupts light flow from the source at high modulation or switching rate such as 20 MHz rate. By switching the laser light source 202, the coherence of the laser light emitted from the laser light source 202 may be reduced, thereby reducing speckle.
  • the scanner 222 redirects or scans the collimated light beam 238 to form a scanned light beam 240 having a position that may vary over time.
  • the scanned beam 240 is directed by the scanner 222 to the F-theta lens 228.
  • the scanner 222 redirects the collimated light beam across two axes where each axis is substantially perpendicular to the axis of the collimated light beam 238.
  • the scanned light beam 240 may be scanned in at least two or more axes.
  • the scanner 222 includes a first reflector 224 and a second reflector 226.
  • the first and second reflectors 224, 226 may comprise optical mirrors or surfaces capable of reflecting undiffused light to form an image.
  • Each reflector 224, 226 may be rotatably coupled with a respective motor 244, 246.
  • Each motor 244, 246 may comprise a galvo drive motor, or the like, that controls a rotational movement of the respective reflector 244, 226 to effect the scanning of the collimated light beam 238.
  • the first and second reflectors 224, 226 may have essentially perpendicular axes, and may be essentially orthogonal with respect to each other.
  • the reflectors 224, 226 also may be positioned at an arbitrary angle relative to each other. Additional reflectors may also be included.
  • the reflectors 224, 226 may be positioned orthogonally so that the collimated laser beam 238 incident on the reflectors may be scanned or redirected in at least two axes.
  • the first reflector 224 scans the beam along one axis, such as an x-axis.
  • the second reflector 226 may be positioned so that the beam along the x-axis incident upon the second reflector 226 may be scanned along an orthogonal direction to the x-axis, such as a y-axis.
  • the first and second reflectors 224, 226 may be positioned orthogonal with respect to each other so that the first reflector scans the beam along the x-axis and the second reflector 226 scans the beam along an orthogonal direction to the x-axis, such as a y-axis.
  • the first reflector 224 also may comprise a spinning polygon mirror such that the rotatable second reflector 226 and the spinning polygon reflector 224 together also are configured to scan the laser beam in two axes.
  • the spinning polygon mirror 224 may scan the collimated light beam 238 along an x-axis and the rotatable mirror 226 may scan the collimated light beam along a y-axis.
  • Each axis, the x-axis and y-axis may be substantially orthogonal with one another, thereby generating a scanned light beam 240 from the collimated beam 238 where the scanned light beam 240 is scanned along two substantially orthogonal axes.
  • the scanner 222 also may include a programmable position controller.
  • the position controller may be a component of the scanner 222 or may be incorporated with the processor 236. By incorporating the position controller with the scanner 232, computing resources of the processor 236 are available for other functions such as processing the image data or for more advanced processing.
  • the position controller may comprise a commercially available controller such as the GSI Lumonics SC2000 Scanner Motion Controller which controls the scanning of the two reflector.
  • the controller may be configured to control the movement of the reflectors 224, 226 by controlling the motors 244, 246.
  • the controller control the movement of the reflectors 224, 226 so that the collimated laser beam 238 is redirected to provide to a desired scan sequence.
  • a coordinate system for the scanner 222 is referred to as X'Y'Z'.
  • the scanned beam 240 is incident to the F-Theta lens 228.
  • the F-theta lens The F-theta lens
  • the 228 focuses the scanned beam 240 to a point or dot.
  • the object 220 to be imaged is positioned within a field of view of F-Theta lens and the image capture instrument 230.
  • the F-theta lens 228 has an optical axis at an angle ⁇ with respect to an optical axis of the image capture instrument 230 so that when the focused dot is scanned across the surface of the object 220 the light is reflected towards the image capture instrument at angle ⁇ .
  • the scanner 222 moves the scanned beam 240 so that the focus point of the laser dot from the F-Theta leans 228 traverses through a pattern across the surface of the object 220.
  • the F-Theta lens 228 may be any commercially available lens such as part number 4401-206-000-20 from Linos, having a 160 mm focal length, a 140 mm diagonal scanning length, +/- 25 degree scanning angle and 633 nm working wavelength.
  • the image capture instrument 230 may be configured and/or positioned to have a field of view that includes the focused laser dot projected on the object 220.
  • the image capture instrument 230 detects the laser dot as it is scanned across the surface of the object 220.
  • the image capture instrument 230 may be sensitive to the light reflected from the object 220. Based on a light detected from the object 220, the image capture instrument generates an electrical signal representative of the surface characteristics (e.g., the contours, shape, arrangement, composition, etc.) of the object 220.
  • the image capture instrument 230 may include an imaging lens 232 and an image sensor 234.
  • the imaging lens 232 is configured to focus the light reflected from the object 220 towards the image sensor 234.
  • the imaging lens 232 may be a telecentric lens configured to minimize perspective errors.
  • the imaging lens 232 may have an internal stop configured to image mostly parallel rays incident at a lens aperture to reduce or eliminate an effect of magnification and perspective correction.
  • the imaging lens 232 may be any commercially available lens configured to minimize perspective distortions such that a lateral measurement on the image of an object does not depend on the distance of the object from the lens such as the China Daheng Corp. combination with front lens number GCO-2305 (50 mm diameter) and the back lens number GCO-2305 (8 mm diameter) where the back lens corresponds to the imaging capture instrument sensor size.
  • the image sensor 234 captures an image of the scanned surface of the object.
  • the image sensor 234 may be a photo-sensitive or light sensitive device or electronic circuit capable of generating signal representative of intensity of a light detected.
  • the image sensor 234 may include an array of photodetectors.
  • the array of photodetectors may be a charge coupled device ("CCD") or a CMOS imaging device, or other array of light sensitive sensors capable of generating an electronic signal representative of a detected intensity of the light.
  • the image sensor 234 may comprise a commercially available CCD or CMOS high resolution video camera having imaging optics, with exposure, gain and shutter control, such as Model SI-3170-CL from Silicon Imaging of Troy, New York.
  • the image sensor 234 also may include a high bandwidth link to a framegrabber device, such as the PIXCI CL1 capture and control computer board from Epix, Inc.
  • Each photodetector of the array generates an electric signal based on an intensity of the light incident or detected by the photodetector. In particular, when light is incident to the photodetector, the photodetector generates an electrical signal corresponding to the intensity of the light.
  • the array of photodetectors includes multiple photodetectors arranged so that each photodetector represents a picture element, or pixel of a captured image. Each pixel may have a discrete position within the array.
  • the image capture instrument 230 may have a local coordinate system, XY such that each pixel of the scanned pattern corresponds to a unique coordinate (x,y).
  • the array may be arranged according to columns and rows of pixels or any other known arrangement.
  • CMOS image sensor may be configured to have an array of light sensitive pixels. Each pixel minimizes any blooming effect such that a signal received by a pixel does not bleed into adjacent pixels when the intensity of the light is too high.
  • the scanner 222 may be configured to scan the laser beam 240 across the surface of the object 220 via the F-Theta lens 228 in many desired patterns.
  • the pattern may be selected to cover a sufficient portion of the surface of the object 220 during a single exposure period.
  • the pattern may also comprise one or more curves or any known pattern from which the characteristics, elevations and configurations of the surface of the object 220 may be obtained.
  • an image of a portion of the surface of the object is captured.
  • the beam 240 scan the object 220 via the scanner 222 and the F-Theta lens 228 in a selected pattern, allowing the imaging sensor 230 to detect the light reflected from object 220.
  • the image sensor 230 generates data representative of the surface characteristics, contours, elevations and configurations of the scanned portion or captured image.
  • the data representation may be stored in an internal or external device such as a memory.
  • the beam 240 is scanned in a pattern across an adjacent portion of the object 220 and an image of the adjacent portion is captured.
  • the scanned beam 240 may scan a different area of the surface of the object 220 during subsequent exposure periods. After a several exposure periods in which the beam 240 is scanned across the various portions of the object 220 and images of those scanned portions captured, a substantial portion of the object may be captured.
  • the processor 236 is coupled to the image capture instrument 230 and configured to receive the signals generated by the image capture instrument 236 that represent images of the scanned pattern on the object 220.
  • the processor 236 also may be coupled to the laser light source and control selected or programmed applications of the laser light.
  • the processor 236 also may be coupled with the scanner 222 and programmed to control the scanning of the collimated light 238.
  • Figure 3 illustrates an example of a scanned pattern of light 348 as viewed from a substantially flat surface.
  • the scanned pattern 348 may include multiple curves 350-355 that are generated by the scanner 222.
  • a portion of the curves 350-351 may be essentially parallel to each other.
  • the curves 350-355 also may represent or include a connected series of points or curvilinear segments where a tangent vector n at any single point or segment obeys the following rule:
  • R is a triangulation axis that is substantially parallel to Y and Y' and passes through an intersection of an axial ray from the image capture instrument 230 and an axial ray from the optical scanner 222. Accordingly, the angle between the tangent n at any point or segment of the curve and the triangulation axis R is not 90 degrees.
  • Each curve 350-355 also may have a cross-sectional intensity characterized by a function that may have a sinusoidal variation, a Gaussian profile, or any other known function for cross-sectional intensity. In an embodiment, a minimum angle between a valid ray between the scanner 222 relative to a valid axial ray of the image sensor 234 is non-zero.
  • the image capture instrument 230 may be characterized by a local coordinate system XYZ, where the X and Y coordinates may be defined by the image capture instrument 230.
  • a value for the Z coordinate may be based on the distance di and d 2 so that l ⁇ z ⁇ 2 .
  • a point from a projected curve incident to a plane perpendicular to Z will appear to be displaced in the X direction by &* . Based on a triangulation angle, the following condition may exist:
  • Tan ⁇ (2) For a given curve (e.g. curve 350) in the projection pattern there may be unique relations ⁇ (y), z base (y) and x base (y).
  • the relations ⁇ (y), z base (y) and x base (y) relations may be determined through calibration.
  • the calibration may be perforated for example by observing the curve 350 as projected on a plane surface.
  • the plane surface may be perpendicular to the image capture instrument 230 at two or more distances d along the Z axis from the image capture instrument 230.
  • ⁇ z 2 , ⁇ z may be computed as ⁇ z
  • a value ⁇ x may be observed using the image capture instrument 230.
  • ⁇ (y) may be computed.
  • the corresponding value z base (y) may be set equal to z ⁇
  • the corresponding value x base (y) may be equal to an x value at the point y on the curve corresponding to z . Additional curves may be used to improve accuracy of through averaging or interpolation.
  • Figure 4 illustrates the scanned pattern of light 448 incident to the object
  • FIG. 5 illustrates the light pattern reflected from the object 420 as incident to the image sensor 534.
  • each curve corresponds to one of the curves 450-455 shown in Figure 4 and a corresponding one of the curves 350-355 shown Figure 3.
  • the corresponding relations ⁇ (y), z base (y) and x base (y) may be selected that were precomputed during a calibration.
  • Equation (2) may be used to determine ⁇ z using ⁇ (y obserVed )- and consequently
  • a maximum displacement for a curve may be determined by:
  • the number " max increases with a decreasing depth of field ' ⁇ 2 and increases with a smaller ⁇ raa .
  • the accuracy of the determination also may decrease with a smaller max values.
  • Figure 6 illustrates an example of an object positioner 660.
  • the positioner 660 is configured to secure and position an object 620 to be imaged in the field of view of the scanned laser beam 240 and the image capture instrument 230.
  • the positioner 660 may include two or more rotary axes to provide for rotation of the object 620.
  • the object 620 may be rotated with respect to the coordinate system XYZ of the image capture instrument 230.
  • the positioner 660 also may include a linear axis to linearly adjust the object 620 to a focal point for the scanning system and image capture unit 230 system.
  • the positioner 660 also may include a platform 664 and a spring loaded clamp 662.
  • the spring-loaded 662 clamp may be configured to securely hold a dental mold or dental casting 620.
  • the clamp 662 also may have magnets (not shown) so that it may be rigidly secured through magnetic attraction to the positioning platform 664.
  • This object 620 may be quickly positioned with the laser imaging system by securing it into the clamp 662 and placing the clamp onto the platform 664. The object 620 may be moved or adjusted with respect to the platform 664 to a desired the position appropriate for digitizing the region of interest.
  • An example of the laser imaging system described above may include a three-dimensional imaging system having a light source and circularizing optics.
  • the light or laser transmitted from the source may be modulated at high frequency for the purpose of reducing the coherence of the laser source and thus reducing the amount of speckle received by the imaging system.
  • the system may include a variable beam expander, a multi-axis scanner system and a flat field scan lens.
  • An image capture instrument may be focused to an area in which an object may be positioned by an adjustable positioner.
  • the image capture system may include a telecentric imaging lens and CMOS imaging sensor.
  • the adjustable positioner may secure dental items such as a dental mold, impressions, or castings.
  • the dental item may be secured using a device such as a spring tensioned vise having magnets for securing the vise to a platform. The vise may be freely moved on and around the platform while holding the dental item solid in a desired position.

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  • Health & Medical Sciences (AREA)
  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Animal Behavior & Ethology (AREA)
  • Public Health (AREA)
  • Computer Vision & Pattern Recognition (AREA)
  • Oral & Maxillofacial Surgery (AREA)
  • Dentistry (AREA)
  • Epidemiology (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Engineering & Computer Science (AREA)
  • General Health & Medical Sciences (AREA)
  • Optics & Photonics (AREA)
  • Veterinary Medicine (AREA)
  • Length Measuring Devices By Optical Means (AREA)
  • Dental Tools And Instruments Or Auxiliary Dental Instruments (AREA)
  • Radiation-Therapy Devices (AREA)
  • Lasers (AREA)
  • Image Processing (AREA)
  • Image Analysis (AREA)
PCT/US2003/041701 2002-12-31 2003-12-30 Laser digitizer system for dental applications Ceased WO2004061389A1 (en)

Priority Applications (6)

Application Number Priority Date Filing Date Title
JP2004564915A JP2006514739A (ja) 2002-12-31 2003-12-30 歯科用レーザデジタイザシステム
DE60326881T DE60326881D1 (de) 2002-12-31 2003-12-30 Digitalisierungssystem mit einem laser für zahntechnische anwendungen
DK03800393T DK1579171T3 (da) 2002-12-31 2003-12-30 Laserdigitizersystem til dentale anvendelser
CA002511828A CA2511828C (en) 2002-12-31 2003-12-30 Laser digitizer system for dental applications
EP03800393A EP1579171B1 (en) 2002-12-31 2003-12-30 Laser digitizer system for dental applications
AU2003300135A AU2003300135B2 (en) 2002-12-31 2003-12-30 Laser digitizer system for dental applications

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
US43737302P 2002-12-31 2002-12-31
US60/437,373 2002-12-31

Publications (1)

Publication Number Publication Date
WO2004061389A1 true WO2004061389A1 (en) 2004-07-22

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PCT/US2003/041701 Ceased WO2004061389A1 (en) 2002-12-31 2003-12-30 Laser digitizer system for dental applications

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US (1) US7142312B2 (enExample)
EP (1) EP1579171B1 (enExample)
JP (1) JP2006514739A (enExample)
AT (1) ATE426793T1 (enExample)
AU (2) AU2003300135B2 (enExample)
CA (1) CA2511828C (enExample)
DE (1) DE60326881D1 (enExample)
DK (1) DK1579171T3 (enExample)
ES (1) ES2324658T3 (enExample)
WO (1) WO2004061389A1 (enExample)

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ATE426793T1 (de) 2009-04-15
EP1579171A1 (en) 2005-09-28
AU2009227412B2 (en) 2011-12-22
US7142312B2 (en) 2006-11-28
JP2006514739A (ja) 2006-05-11
DE60326881D1 (de) 2009-05-07
CA2511828A1 (en) 2004-07-22
DK1579171T3 (da) 2009-07-20
ES2324658T3 (es) 2009-08-12
EP1579171B1 (en) 2009-03-25
AU2003300135B2 (en) 2009-07-16
CA2511828C (en) 2008-12-09
AU2003300135A1 (en) 2004-07-29
US20040201856A1 (en) 2004-10-14

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