METHOD AND SYSTEM FOR MEASURING GEOMETRIC PARAMETERS OF THROUGH HOLES

Abstract

A method of measuring geometric parameters of through holes in a thin substrate includes acquiring images of select sub-volumes of the substrate using an optical system having a field of depth greater than a thickness of the substrate. The acquired images are processed to determine the desired geometric parameters.

Claims

1. A method of measuring geometric parameters of through holes in a substrate, comprising: positioning a camera comprising an image sensor and a lens having a depth of field greater than a thickness of the substrate at a measuring station; positioning a select sub-volume of the substrate within a field of view of the camera and within the depth of field; illuminating the select sub-volume; capturing an image of the select sub-volume on the image sensor; and processing the image to determine at least one geometric parameter of at least one through hole in the select sub-volume.

2. The method of claim 1, wherein the at least one geometric parameter is a clear aperture size of the at least one through hole.

3. The method of claim 1, wherein the substrate has a thickness of 1 mm or less.

4. The method of claim 1, wherein the lens is a telecentric lens.

5. The method of claim 1, wherein the illuminating the select sub-volume comprises using collimated light.

6. The method of claim 1, wherein the select sub-volume has a front side and a back side, wherein positioning the select sub-volume comprises positioning the front side in opposing relation to the lens, and wherein illuminating the select sub-volume comprises directing light at the front side of the select sub-volume.

7. The method of claim 6, wherein directing the light at the front side of the select sub-volume comprises passing a light beam through the lens to the front side of the select sub-volume.

8. The method of claim 6, wherein illuminating the select sub-volume further comprises reflecting the light into the select sub-volume using a mirror mounted at the back side of the select sub-volume.

9. The method of claim 1, wherein the select sub-volume has a front side and a back side, wherein positioning the select sub-volume comprises positioning the front side in opposing relation to the lens, and wherein illuminating the select sub-volume comprises directing light at the back side of the select sub-volume.

10. The method of claim 1, further comprising effecting a relative motion between the camera and the substrate to position another sub-volume of the substrate within the field of view of the camera and within the depth of field.

11. The method of claim 10, further comprising illuminating the another sub-volume with light, capturing an image of the another sub-volume on the image sensor, and processing the image of the another sub-volume to determine at least one geometric parameter of at least one hole in the another sub-volume.

12. The method of claim 11, wherein illuminating the another sub-volume comprises effecting a relative motion between a source of the light and the substrate such that the another sub-volume is within an illumination volume of the light.

13. The method of claim 1, wherein processing the image comprises detecting changes in contrast in the image.

14. A system for measuring geometric parameters of through holes in a substrate, comprising: a camera comprising an image sensor and a lens having a depth of field greater than a thickness of the substrate, the camera positioned at a select working distance relative to the substrate such that a select sub-volume of the substrate is within a field of view of the camera and within the depth of field; a lighting arrangement for illuminating the select sub-volume; and a processor configured to receive image data from the camera and determine from the image data at least one geometric parameter of at least one through hole in the select sub-volume.

15. The system of claim 14, wherein the lens is a telecentric lens.

16. The system of claim 14, wherein the lighting arrangement is a collimated lighting arrangement.

17. The system of claim 14, wherein the select sub-volume has a front side and a back side, wherein the front side is in opposing relation relative to the lens, and wherein the lighting arrangement comprises a light source positioned to direct a light beam at the back side of the select sub-volume.

18. The system of claim 14, wherein the select sub-volume has a front side and a back side, wherein the front side is in opposing relation to the lens, and wherein the lighting arrangement comprises a coaxial light source optically coupled to the lens.

19. The system of claim 18, wherein the lighting arrangement further comprises a mirror mounted in contact with a back side of the select sub-volume.

20. The system of claim 19, wherein the mirror extends across a back side of the substrate including the back side of the select sub-volume.

21. The system of claim 14, further comprising a translation mechanism coupled to the substrate and operable to translate the substrate relative to the camera.

22. The system of claim 14, wherein the processor is configured to determine a clear aperture size of the at least one through hole from the image data.

Description

BRIEF DESCRIPTION OF DRAWINGS

[0027] The following is a description of the figures in the accompanying drawings. The figures are not necessarily to scale, and certain figures and certain views of the figures may be shown exaggerated in scale or in schematic in the interest of clarity and conciseness.

[0028] FIG. 1A is a cross-section of an example substrate having through holes.

[0029] FIG. 1B is a top view of the substrate shown in FIG. 1A.

[0030] FIG. 2A is a diagram of a system for measuring geometric parameters of through holes in a substrate.

[0031] FIG. 2B is a top view of the system shown in FIG. 2A.

[0032] FIG. 3 is an image of a hole acquired by the method of FIG. 1.

[0033] FIG. 4 is a diagram of another system for measuring geometric parameters of through holes in a substrate.

[0034] FIG. 5A is an image of a select sub-volume of a substrate acquired without using telecentric optics.

[0035] FIG. 5B is an image of a select sub-volume of a substrate acquired with use of telecentric optics.

[0036] FIG. 6A is a close-up view of section 6A of FIG. 5A.

[0037] FIG. 6B is a close-up view of section 6B of FIG. 5B.

DETAILED DESCRIPTION

[0038] To provide a context for the method and system disclosed herein, FIGS. 1A and 1B illustrate geometric parameters of example through holes 10 formed in an example substrate 12. The through holes 10 are holes that run along the thickness (T) of the substrate 12 or from the front side 12A of the substrate 12 to the back side 12B of the substrate 12. Along the thickness (T) of the substrate 12, i.e., along the Z axis, the through holes 10 may have any desired shape, such as straight, tapered, or hourglass. In the plane of the substrate 12, i.e., in the XY plane, the through holes 10 may have any desired cross-sectional shape, such as circular, square, or elliptical. One of the hole geometric parameters that may be measured is clear aperture size. The clear aperture of a through hole is the aperture of the path through the through hole where light can travel unobstructed. The clear aperture size of a through hole 10 may be defined as the minimum distance diameter, or minimum transverse dimension, (C) of the through hole 10. Examples of other hole geometric parameters that may be measured are maximum diameter (d1) of the through hole 10, average diameter of the through hole 10, aspect ratio of the through hole 10, and direction of a major axis of the through hole 10.

[0039] FIG. 2A shows a measurement system 101 including an imaging apparatus 104 for acquiring images of through holes in a substrate according to one embodiment. The images acquired by the imaging apparatus 104 can be processed to determine any of the hole geometric parameters discussed above. For illustration purposes, FIG. 2A shows a sample substrate 100 having through holes 102 and a thickness T1, which is also the depth of the through holes 102. Although only a few through holes 102 are shown in the substrate 100, more commonly, a sample substrate will have numerous through holes, e.g., ranging from tens to thousands of holes. The measurement system 101 is not limited to any number of through holes in the substrate 100. Although the through holes 102 are shown as straight holes having a circular cross-section (see FIG. 2B), the measurement system of 101 is also not limited to any particular shape of through holes or orientation of through holes in the substrate. The through holes in the substrate 100 may have any of the shapes discussed above and other shapes not specifically mentioned above. In one embodiment, the substrate 100 is a thin substrate having a thickness of 1 mm or less, although the thickness of the substrate will generally only be limited by the depth of field of the imaging apparatus 104. In FIG. 2A, the through holes 102 are exaggerated in size (diameter) relative to the field of view of the imaging apparatus 104. For most applications justifying the cost of the measurement system, the through holes 102 in the sample substrate 100 will typically be micron-sized, although the size of the through holes 102 will generally only be limited by the field of view and the resolution of the imaging apparatus 104.

[0040] In one embodiment, the imaging apparatus 104 includes a camera 106 and a backlight illuminator 108 arranged on opposite sides of the substrate 100, and particularly on opposite sides of a target sub-volume 109 of the substrate 100. The target sub-volume 109 includes one or more through holes 102 whose geometric parameters are to be measured. In one embodiment, the camera 106 includes an image sensor 110 and an objective lens 112 optically coupled to the image sensor 110. In one embodiment, the image sensor 110 has a pixel count of at least 10 megapixels (MP), allowing the camera 106 to capture high resolution images. However, the size of the image sensor 110 will generally be dictated by the desired accuracy of the measurement. For example, if a 100 micron geometric feature is to be measured with 1 micron accuracy, the image pixel size should be close to 1 micron. Image pixel size is a function of the physical size of the image sensor pixel and the magnification of the objective lens. In some embodiments, the objective lens 112 is a telecentric lens. Reasons for selecting a telecentric lens as the objective lens 112 are discussed below.

[0041] Conventional lenses have angular fields of view, which means that as the distance between the lens and object increases, the magnification decreases. This angular field of view results in parallax error, also known as perspective error. Telecentric lenses eliminate this parallax error by having a constant, non-angular field of view. With telecentric lenses, magnification remains constant with object displacement, provided the object stays within the telecentric range. The term “telecentric range” or “telecentric depth” or “depth of field (DOF)”, as used with telecentric lenses, refers to the total distance above and below an object that remains in focus and at constant magnification. Telecentric range may be defined as a range of axial displacements causing a variation in image size of less than 1 micron. The telecentric range (or telecentric depth or DOF) of a telecentric lens can be obtained from the lens manufacturer or may be included in the specification of the telecentric lens.

[0042] By using a telecentric lens as the objective lens 112, according to one embodiment, virtually distortion free images can be acquired and used to accurately determine the desired geometric parameters of the through holes in the substrate 100. In one embodiment, the telecentric objective lens 112 has a telecentric range (TR in FIG. 2A), that is greater than the thickness T1 of the substrate 100. A procedure for selecting the telecentric objective lens 112 may include finding telecentric lenses from commercial sources (for example Opto Engineering) that meet the telecentric range requirement stated above. From this set of telecentric lenses, the telecentric lens with the highest magnification can be selected for use as the telecentric objective lens 112. For measurement of hole geometric parameters using the selected telecentric lens, the working distance WD, which is the distance between the front surface of the telecentric lens 112 and the front surface 100A of the substrate 100, is adjusted such that the target sub-volume 109 of the substrate 100 lies entirely within the telecentric range. The manufacturer's specification for the telecentric lens will typically include the working distance for the selected magnification and telecentric range (or DOF or telecentric depth).

[0043] In one embodiment, the backlight illuminator 108 is used to produce a sharp silhouetted image of the holes to be measured. For the telecentric lens 112, the backlight illuminator 108 can be a telecentric illuminator, which is a collimated illuminator that is designed to work specifically with telecentric lenses. Telecentric illuminators are available commercially (for example, from Opto Engineering). The telecentric illuminator 108 will uniformly illuminate the target sub-volume 109 of the substrate 100 with a collimated light beam. The illumination volume must be the size of the target sub-volume 109 or bigger to assure illumination of the entire field of view. For the arrangement shown in FIG. 2A, the optical axes of the backlight illuminator 108 and telecentric lens 112 are aligned. The distance BD of the backlight illuminator 108 from the back surface 100B of the substrate 100 may be selected to achieve a desired illumination of the target sub-volume 109 of the substrate 100.

[0044] FIG. 3 shows an example of a silhouetted image, where the through hole in the target sub-volume appears as a light spot 120 surrounded by a dark ring 122 in a transparent substrate 124. The dark ring 122 is the superimposed area of sidewalls as seen when looking into the hole. The more the sidewalls are tapered and distinctly different from a cylinder, the thicker the dark ring will appear in the image. For a straight hole, the diameter 126 of the light spot 120 will indicate the clear aperture size of the hole. The clear aperture size can be measured by counting the pixels corresponding to the diameter 126.

[0045] FIG. 4 shows a modified system 101A including a different lighting arrangement that may be used with the telecentric lens 112. The different lighting arrangement includes a coaxial light source 130 arranged on the same side of the substrate 100 as the camera 106′. The coaxial light source 130 may include a light source 130A and optics module 130B for aligning the light from the light source 130A in a direction generally parallel to the optical axis 115 of the telecentric lens 112. For example, the optics module 130B may include a beam splitter. The optics module 130B may be arranged in line with the telecentric lens 112 and image sensor 110, as shown in FIG. 4. The different lighting arrangement may further include a mirror 134 arranged in contact with the back surface 100B of the substrate 100. The mirror 134 will reflect the light from the optics module 130B into the target sub-volume 109 of the substrate 100 to be measured. The mirror 134 may extend across the back surface 100B of the substrate 100 and may be movable with the substrate 100 as a unit.

[0046] Both the lighting arrangements shown in FIGS. 2A and 4 can be used when measuring through hole parameters in transparent substrates such as glass. Both the lighting arrangements shown in FIGS. 2A and 4 are also suitable for use with opaque substrates. However, the lighting arrangement shown in FIG. 2A may work better for opaque substrates due to its higher contrast. The lighting arrangement shown in FIG. 4 has an advantage when there is no access to the back side of the substrate, such as when the substrate sits in a solid chuck, or when there is insufficient room behind the back side of the substrate to put the backlight illuminator.

[0047] Returning to FIG. 2A, the field of view of the camera 106 (106′ in FIG. 4) is limited to the diameter of the front surface of the telecentric lens 112 (i.e., the surface of the lens in opposed relation to the substrate 100). The field of view of the camera 106 (106′ in FIG. 4) and the telecentric range of the telecentric lens 112 define the target sub-volume of the substrate whose image is acquired at any moment. However, scanning of the substrate will allow all the holes in the substrate or all the holes within a desired volume of the substrate to be measured. Scanning involves providing relative motion between the substrate 100 and the imaging apparatus 104. In one embodiment, the camera 106 and backlight illuminator 108 (or camera 106′ and coaxial light source 130 in the embodiment of FIG. 4) may be held in fixed positions while the substrate 100 is translated in a plane perpendicular to the optical axis 115 of the camera 106 (i.e., the XY plane as shown in FIG. 2B). This will allow different sub-volumes of the substrate 100 to be moved into the field of view of the camera 106 over the scanning period. A translation stage 117 may be coupled to the substrate 100 and operated to translate the substrate 100 in the desired directions or plane. It is also possible to hold the substrate 100 fixed while translating the camera 106 and backlight illuminator 108 (or camera 106′ and coaxial light source 130 in the embodiment of FIG. 4) relative to the substrate 100.

[0048] A controller 140 may be coupled to the camera 106 (106′ in FIG. 4) to receive image data from the camera 106. The controller 140 may include a memory device 142 for storing the received image data and a processor 144 for processing the image data. The processor 144 may be configured to process the image data to determine one or more geometric parameters, such as clear aperture size, of through holes represented in the image data. The processor 144 may run a commercially available image processing software capable of analyzing the image data and extracting the desired geometric parameters from the image data. Examples of suitable commercial image processing software packages include, but are not limited to, HALCON by MVTec Software GmbH, MATLAB by MathWorks, Matrox Inspector with Matrox Imaging Library by Matrox, and NI Vision by National Instrument. The measured geometric parameters may be stored in the memory device 142 or other suitable storage device for later use. The controller 140 may also control translation of the substrate 100 during scanning of the substrate 100. For example, after processing the image data acquired by the camera 106 (106′ in FIG. 4) for a current target sub-volume, the processor 144 may issue a command to the translation stage 117 to move the next target sub-volume into the field of view of the camera 106 (camera 106′ for the embodiment in FIG. 4).

[0049] Table 1 below shows examples of telecentric lens options for acquiring images of through holes in thin substrates.

TABLE-US-00001 TABLE 1 Lens Telecentric Field of Magni- range or Camera View Pixel Size Option fication DOF (mm) Array (mm) (microns) 1 1X 0.9 3840 × 2748 6.4 × 4.8 1.7 2   1.33X 0.5 3840 × 2748 4.8 × 3.6 1.3 3 2X 0.2 3840 × 2748 3.2 × 2.4 0.85

[0050] FIG. 5A shows an image of 3×4 holes acquired with VIEW Summit 650 Optical Coordinate Measuring Machine (OCMM). FIG. 5B shows an image of 3×4 holes acquired with a 10 megapixels camera using telecentric optics as listed in Option 1 in Table 1. Both images in FIGS. 5A and 5B were taken at 1X optical magnification with green backlighting. For the image in FIG. 5B, the backlight was a telecentric (i.e., collimated) light source. FIG. 6A shows a zoomed-in view of four of the holes in FIG. 5A. FIG. 6B shows a zoomed-in view of four of the holes in FIG. 5B. The image in FIG. 6B, which was acquired with telecentric optics, shows a much more defined outline of the holes than the image in FIG. 6A, which was acquired with the OCMM. The much smaller depth of field in the OCMM measurement system used to acquire the image of FIG. 6A prevented waists at different depths from being in focus simultaneously.

[0051] A procedure for measuring one or more geometric parameters of through holes in a substrate may include selecting the lens objective for a particular substrate thickness. Examples of lens objectives are given in Table 1. After the lens objective has been selected, the desired geometric parameters, such as clear aperture size, of holes in the substrate can be measured quickly in a few simple steps, as outlined below.

[0052] The substrate is moved in between the backlight illuminator 108 and the camera 106 for the system shown in FIG. 2A (or beneath the coaxial light source 130 and camera 106′ for the system shown in FIG. 4) to position a target sub-volume of the substrate in the field of view of the camera.

[0053] The target sub-volume is illuminated, and an image of the illuminated target sub-volume is acquired.

[0054] The acquired image is processed to determine at least one geometric parameter of each through hole in the target sub-volume. Processing involves detecting changes in light levels, or contrast, in the acquired image. Changes in contrast can define boundaries, or lines, within the image. These lines can be extended to create objects like segments, circles, ellipses, and the like, and then parameters such as diameter or distance can be extracted. The acquired image is typically processed on a computer using commercially available image analysis software. Examples of suitable commercial imaging processing software packages include, but are not limited to, HALCON by MVTec Software GmbH, MATLAB by MathWorks, Matrox Inspector with Matrox Imaging Library by Matrox, and NI Vision by National Instrument.

[0055] The geometric parameter values for each hole are recorded. The acquired image may be discarded after recording the geometric parameter values to save storage space since the high-resolution images can be quite large.

[0056] The substrate is then translated relative to the camera and lighting arrangement to place another target sub-volume of the substrate in the field of view of the camera and within the illumination volume provided by the lighting arrangement. The acquiring of the image of the target sub-volume, processing of the image, and recording of geometric parameter values for each hole in the target sub-volume are repeated for the new target sub-volume.

[0057] The procedure described above can be automated to scan an entire substrate or a small area within the substrate. The duration of a measurement run is determined predominantly by how fast the substrate can be translated and how fast the images can be acquired and processed and not by the number of holes in the field of view. A substrate with holes ranging from hundreds to thousands can be quickly measured using an automated procedure and any of the setups described in FIGS. 2A and 4. In some embodiments, multiple cameras 106, 106′ may be utilized to increase the speed of scanning the substrate. In some embodiments, multiple illuminator 108 may be used in conjunction with the multiple cameras. In some embodiments, there may be constant relative movement between the substrate and cameras 106, 106′ and illuminator 108 or light source 130 may turn on and off (e.g., strobe) at regular intervals for cameras 106, 106′ to take images.

[0058] While the invention has been described with respect to a limited number of embodiments, those skilled in the art of, having benefit of this disclosure, will appreciate that other embodiments can be devised which do not depart from the scope of the invention as disclosed herein. Accordingly, the scope of the invention should be limited only by the accompanying claims.