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WO2003069384A1 - Fiber optical plate and irregular pattern detection device - Google Patents

Fiber optical plate and irregular pattern detection device Download PDF

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Publication number
WO2003069384A1
WO2003069384A1 PCT/JP2003/001587 JP0301587W WO03069384A1 WO 2003069384 A1 WO2003069384 A1 WO 2003069384A1 JP 0301587 W JP0301587 W JP 0301587W WO 03069384 A1 WO03069384 A1 WO 03069384A1
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WO
WIPO (PCT)
Prior art keywords
illumination
core
light
fiber
area
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/JP2003/001587
Other languages
French (fr)
Japanese (ja)
Inventor
Takeo Sugawara
Yoshio Natsume
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.)
Hamamatsu Photonics KK
Original Assignee
Hamamatsu Photonics KK
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 Hamamatsu Photonics KK filed Critical Hamamatsu Photonics KK
Priority to AU2003212007A priority Critical patent/AU2003212007A1/en
Publication of WO2003069384A1 publication Critical patent/WO2003069384A1/en
Anticipated expiration legal-status Critical
Ceased legal-status Critical Current

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Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01BMEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
    • G01B11/00Measuring arrangements characterised by the use of optical techniques
    • G01B11/24Measuring arrangements characterised by the use of optical techniques for measuring contours or curvatures
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B6/00Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
    • G02B6/04Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings formed by bundles of fibres
    • G02B6/06Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings formed by bundles of fibres the relative position of the fibres being the same at both ends, e.g. for transporting images
    • G02B6/08Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings formed by bundles of fibres the relative position of the fibres being the same at both ends, e.g. for transporting images with fibre bundle in form of plate
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B6/00Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
    • G02B6/24Coupling light guides
    • G02B6/26Optical coupling means
    • G02B6/262Optical details of coupling light into, or out of, or between fibre ends, e.g. special fibre end shapes or associated optical elements
    • GPHYSICS
    • G06COMPUTING OR CALCULATING; COUNTING
    • G06VIMAGE OR VIDEO RECOGNITION OR UNDERSTANDING
    • G06V40/00Recognition of biometric, human-related or animal-related patterns in image or video data
    • G06V40/10Human or animal bodies, e.g. vehicle occupants or pedestrians; Body parts, e.g. hands
    • G06V40/12Fingerprints or palmprints
    • G06V40/13Sensors therefor
    • G06V40/1324Sensors therefor by using geometrical optics, e.g. using prisms
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B6/00Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
    • G02B6/24Coupling light guides
    • G02B6/42Coupling light guides with opto-electronic elements
    • G02B6/4201Packages, e.g. shape, construction, internal or external details
    • G02B6/4249Packages, e.g. shape, construction, internal or external details comprising arrays of active devices and fibres

Definitions

  • the present invention relates to a fiber optical plate and an uneven pattern detecting device to which the fiber optical plate is applied.
  • a conventional concavo-convex pattern detection device using scattered light inside the object to be measured is disclosed in, for example, Japanese Patent No. 3045629, in which illuminating light enters the inside of the object to be measured from the side, and In some cases, light scattered inside the target is incident on the concave / convex pattern transmission means arranged below the target object. Further, as disclosed in Japanese Patent Application Laid-Open No. 2000-217803, there has been an apparatus in which an illuminating unit arranged on a side of a light receiving element illuminates an object to be measured placed on a light receiving surface of the light receiving element.
  • Japanese Patent No. 3 04 562 9 No. irregular pattern detector publications for illuminating means which is separated from the concave-convex patterns transmission means, the side of the object to be measured, that is, disposed obliquely Me above the detection surface
  • the size or thickness of the device is limited.
  • the uneven pattern detection device disclosed in Japanese Patent Application Laid-Open No. 2000-217803 has a problem that the illumination means cannot efficiently illuminate the object to be measured.
  • the present invention has been made to solve the above-described problems.
  • the device In an uneven pattern detection device using scattered light inside an object to be measured, the device is reduced in size or thickness, and illumination means is efficiently measured.
  • a fiber optic plate and a fiber optic plate that can illuminate an object The purpose is to provide.
  • a fiber optical plate of the present invention is applied to an uneven pattern detecting device for detecting an uneven pattern of a measured object, and each axis crosses both end surfaces obliquely, and a plurality of fibers are formed in a clad.
  • a plurality of optical fibers are aggregated and arranged so that the cores are arranged at predetermined intervals.
  • the molded optical fiber plate is a fiber optical plate, and a detection area facing an imaging means for imaging an uneven pattern is provided. And an illumination area facing illumination means for illuminating the object to be measured, and a light absorber for absorbing light is provided in the cladding in the detection area.
  • the light absorber is provided in the clad, so that the uneven pattern of the measured object is transmitted to the imaging means with high accuracy.
  • the illumination area since no light absorber is provided in the cladding, the illumination light emitted by the illumination means is efficiently guided to the object to be measured.
  • an illumination means is attached to the illumination light incident surface of the fiber optical plate to reduce the size or thickness of the device. It becomes possible to do.
  • the refractive index of the cladding in the illumination region is lower than the refractive index of the cladding in the detection region.
  • Fiber optic plate whose axis obliquely intersects the surface of the fiber optic plate at a predetermined angle (slant angle) so that even if disturbance light in the air enters the core, it will not be totally reflected at the core' cladding interface. Can be emitted only at a portion of the exit surface where an object having a higher refractive index than air is in contact.
  • the critical angle at the core-cladding interface in the illumination region becomes smaller. Therefore, even in the case of a fiber optic plate with a slant angle set so that disturbance light in the air is not guided in the detection area, in the illumination area, total reflection is performed at the core / cladding interface at a small angle (incident angle).
  • the illumination light traveling through the core while The light can be emitted to the outside even at the part of the emission surface that is in contact with the air. As a result, the measured object is illuminated more efficiently.
  • the refractive index of the core in the illumination region is preferably lower than the refractive index of the core in the detection region.
  • the critical angle at the air-core interface in the illumination region increases. Therefore, even in the case of a fiber optical plate in which the axis line and the emission surface obliquely intersect, in the illumination area, the illumination light is easily emitted to the outside even in the portion of the emission surface that is in contact with air. As a result, the measured object is illuminated more efficiently.
  • the interval at which the plurality of cores are arranged in the illumination area is longer than the interval at which the plurality of cores are arranged in the detection area.
  • the thickness of the clad interposed between the cores is not changed.
  • the area ratio of the core on the incident surface of the illumination light can be increased, and the incidence efficiency of the illumination light on the illumination region is improved.
  • the number of cores per unit area on the surface of the detection area increases, and the accuracy of the concavo-convex pattern transmitted in the detection area improves. I do.
  • the uneven pattern detection device of the present invention includes any one of the fiber optical plates, wherein the imaging means is mounted so as to face one surface of the detection area, and the illumination means is arranged with the imaging means of the illumination area. It is attached so as to face the surface on the side to be cut.
  • the uneven pattern detection device of the present invention includes the above-described fiber optical plate, efficient illumination of the object to be measured can be realized, and the device can be mounted by attaching illumination means to the illumination light incident surface in the illumination area. The size or thickness is reduced.
  • FIG. 1 is a plan view of an uneven pattern detecting device 2 to which a fiber optical plate 1 is applied.
  • FIG. 2 is a cross-sectional view taken along the line II-II of the uneven pattern detecting device 2 shown in FIG.
  • FIG. 3 is a sectional view taken along the line III-III of the uneven pattern detecting device 2 shown in FIG.
  • FIG. 4 is a front view of the LED array 5.
  • FIG. 5 is a cross-sectional view of the LED array 5 shown in FIG. 4 along the line VV.
  • FIG. 6 is a front view of the fiber optic plate 1 shown in FIG.
  • FIG. 7 is a partially enlarged cross-sectional view of the fiber optic plate 1 in the detection area 12.
  • FIG. 8 is a diagram showing a state where a finger 6 to be measured is placed on the fiber optical plate 1.
  • FIG. 9 is a view showing a mode in which the illumination light is emitted or reflected on the illumination light exit surface 144. As shown in FIG.
  • FIG. 10 is a diagram illustrating a mode in which the detection light that has entered the detection region 12 from the finger 6 is guided by the optical transmission line in the detection region 12.
  • FIG. 11 is a diagram showing a state in which the illumination light is emitted or reflected on the illumination light exit surface 744.
  • FIG. 12 is a diagram illustrating a mode in which the illumination light is emitted or reflected on the illumination light emission surface 844.
  • FIG. 13 is a conceptual diagram showing a state in which the LED array 20 is attached to the fiber optical plate 10.
  • FIG. 14 is a conceptual diagram showing a mode in which the LED array 60 and the intermediate fiber optical plate 70 are disposed below the illumination light incidence surface 542 with the intermediate fiber optical plate 70 interposed therebetween.
  • FIG. 15 is a conceptual diagram showing a mode in which an intermediate fiber optical plate 70 is interposed between the LED array 60 and the light receiving surface 80 and the fiber optical plate 50.
  • FIG. 16 is a front view of the embedded LED array 9.
  • FIG. 17 is a cross-sectional view of the embedded LED array 9 shown in FIG. 13 taken along the line XIV-XIV.
  • FIG. 1 is a plan view of an uneven pattern detecting device 2 to which a fiber optical plate 1 is applied.
  • FIG. 2 is a cross-sectional view taken along the line II-II of the uneven pattern detecting device 2 shown in FIG.
  • FIG. 3 is a sectional view taken along line III-III of the uneven pattern detection device 2 shown in FIG.
  • the frame 3 has a rectangular bottom surface 32, and four wire terminals 34 on two opposite sides of the bottom surface 32 in the short side direction.
  • the image sensor 4 is installed at the center on the bottom surface 32.
  • the imaging device 4 has a flat plate shape, and the upper portion of the imaging device 4 (hereinafter, the direction in which the imaging device 4 is installed as viewed from the bottom surface 32 is the upper direction, and the opposite direction is the lower portion).
  • the image sensor 4 has a rectangular light receiving surface 42, and an outer frame 44 around the light receiving surface 42 on the upper surface of the image sensor 4.
  • the thickness of the imaging element 4 matches the thickness of the LED array 5 described later.
  • the image pickup device 4 is disposed such that the longitudinal direction of the light receiving surface 42 and the longitudinal direction of the bottom surface 32 match. 2 and 3, a portion corresponding to the light receiving surface 42 of the surface of the image sensor 4 is indicated by a thick line.
  • the image sensor 4 includes four wire terminals 46 on two opposing sides (on the outer frame 44) of the light receiving surface 42 on the outer side in the lateral direction.
  • the image sensor 4 is wired by connecting the wire terminals 46 and the wire terminals 34 of the frame 3 with bonding wires 36.
  • the bottom surface 3 2 of the frame 3 should be adjacent to the image sensor 4 on two opposite sides in the longitudinal direction.
  • LED array 5 is installed.
  • the LED array 5 functioning as an illuminating means has a thin long plate shape, and by applying such a thin illuminating means, the uneven pattern detecting device 2 can be made thin.
  • the LED array 5 is installed such that the length direction coincides with the short direction of the bottom surface 32.
  • FIG. 4 is a front view of the LED array 5.
  • FIG. 5 is a cross-sectional view of the LED array 5 shown in FIG. 4 along the line VV.
  • the LED array 5 includes a long printed board 502 on the bottom surface.
  • a plurality of LEDs 504 are arranged on the printed circuit board 502 along the longitudinal direction of the printed circuit board 502, and a resistor 506 is provided at the end. LED 504 and resistor 506 are wired with lead 508. The entire surface of the printed circuit board 502 on which the LED 504 and the resistor 506 are installed is covered with an epoxy-based transparent resin 510.
  • the fiber optic plate 1 is set on the image sensor 4 and the LED array 5.
  • the surface of the fiber optic plate 1 is rectangular and its length in the short direction matches the length in the long direction of the LED array 5 and is longer than the length in the short direction of the light receiving surface 42 of the image sensor 4 .
  • the fiber optical plate 1 coincides with the longitudinal direction of its surface and the longitudinal direction of the bottom surface 32 of the frame 3, and its surface covers the entire upper surface of the LED array 5 and the entire light receiving surface 42 of the image sensor 4.
  • the terminal 46 is in contact with the terminal 46 and is not installed.
  • the fiber optic plate 1 is composed of a plurality of optical fibers bundled together so that their axes are parallel to each other, and a plurality of cores in a clad.
  • the fiber optical plate 1 is sliced so that the axis (center axis) and the surface (end face) of the fiber optical plate 1 obliquely intersect at an angle (slant angle) ⁇ °. In the present embodiment, both end faces of the fiber optical plate 1 are parallel.
  • the fiber optic plate 1 has a detection area 12 in the center of the surface in the longitudinal direction where the light absorber is arranged in the clad, and an illumination area 14 in which the light absorber is not arranged in the clad at both ends. Is provided.
  • the portion of the fiber optical plate 1 corresponding to the detection area 12 is double oblique.
  • the portion corresponding to the illumination area 14 is indicated by a solid line.
  • an uneven pattern input surface 122 for taking in the scattered light inside the object to be measured is formed, and on the lower surface of the detection area 12, the scattered light (detection light) guided is provided.
  • a projection pattern output surface 124 to be emitted is formed.
  • FIG. 6 is a front view of the fiber optic plate 1 shown in FIG.
  • the dotted area in FIG. 6 indicates the concave / convex pattern input surface 122 of the surface of the fiber optical plate 1, and the portion other than the dotted area indicates the illumination light emitting surface 144.
  • the fiber optical plate 1 is installed such that the entire light receiving surface 42 of the image sensor 4 contacts the concave / convex pattern output surface 124, and the LED array 5 contacts the illumination light incident surface 142.
  • the fiber optic plate 1 and the image sensor 4 and the LED array 5 are joined with a transparent adhesive (epoxy or silicone resin).
  • FIG. 7 is a partially enlarged cross-sectional view of the fiber optic plate 1 in the detection area 12.
  • Each optical transmission line (hereinafter, a portion of the fiber optical plate 1 that is constituted by a core and a clad surrounding the core is referred to as an “optical transmission line”) has a core 160 as a center, and Rad 16 1 closely surrounds core 160. Further, the light absorber 16 2 closely surrounds the clad 16 1. Both ends 16 5 of each optical transmission line are angled (slant angle) with respect to axis 16 4. Incline. This slant angle. The angle is set such that, even when light enters the core 160 from the air, the incident light is not totally reflected at the interface between the core 160 and the clad 161.
  • a predetermined slant angle the light incident on the core 160 from the air is refracted at the air / core interface at a refraction angle of 3 ° when passing through the end face 1650 of the optical transmission line, and then the core's cladding boundary It reaches the core-cladding interface at an angle (incident angle) smaller than the critical angle on the surface.
  • Slant angle ⁇ The specific angle c .
  • ac ° is an angle that satisfies the following equations (1) to (3).
  • n a is the refractive index of air. 6 C ° is the critical angle at the core-cladding interface.
  • the core and the clad constituting the optical transmission line of the illumination region 14 are of the same quality as the core 160 and the cladding 161 constituting the optical transmission line of the detection region 12.
  • MF multi-fiber
  • MMF multi-multi-fiber sensing areas
  • MF multi-fiber
  • MMF multi-multi-fiber sensing areas
  • MF multi-fiber
  • MMF Multi-multi-fiber sensing areas
  • the optical fiber used to manufacture the multi-fiber (MF) or multi-multi-fiber (MMF) for the detection area and the optical fiber used to manufacture the multi-fiber (MF) or multi-multi-fiber (MMF) for the illumination area Phino has the same outer diameter.
  • the multi-fiber (MF) or multi-multi fiber (MMF) for the detection area and the multi-fiber (MF) or multi-multi fiber (MMF) for the illumination area are aligned in the mold by the required height.
  • the optical fiber used to manufacture the multi-fiber (MF) or multi-multi fiber (MMF) for the detection area and the multi-fiber (MF) or multi-multi fiber for the illumination area Since the outer diameter of the optical fiber used in the manufacture of Aiva (MM F) is the same as that of the optical fiber, disturbance at the interface is eliminated.
  • the aligned multi-fiber (M F) or multi-multi-fiber (MM F) is fused in a hot pressing process.
  • the fiber optic plate 1 is completed by slicing and polishing the fused body.
  • FIG. 8 is a diagram showing a state where a finger 6 to be measured is placed on the fiber optical plate 1. As shown in FIG. 8, the finger 6 is placed on the fiber optical plate 1 such that the belly of the finger 6 covers the uneven pattern input surface 122 and the illumination light emission surface 144.
  • the illumination light emitted from the LED array 5 enters the illumination area 14 from the illumination light incident surface 14 2.
  • the illumination light that has entered the illumination area 14 is guided by the optical transmission path of the illumination area 14 and reaches the illumination light exit surface 144.
  • the illumination light that has reached the illumination light exit surface 144 enters the inside of the finger 6 at the portion of the illumination light exit surface 144 that contacts the convex part of the finger 6, and becomes scattered light.
  • the illuminating light that has reached the illuminating light exit surface 1 '44 is a portion of the illuminating light exit surface 144 that is located in the concave portion of the belly of the finger 6, i.e., the air comes into contact with the illuminating light exit surface 144. In the portion, the light is totally reflected by the illumination light exit surface 144.
  • FIG. 9 is a view showing a mode in which the illumination light is emitted or reflected on the illumination light exit surface 144.
  • the end surface 165 a of the optical transmission line shown in FIG. 9 indicates the end surface of the optical transmission line in contact with air
  • the end surface 165 b of the optical transmission line indicates the end surface of the optical transmission line in contact with the finger 6.
  • the illumination light guided by the optical transmission path in the illumination area 14 has a critical angle ⁇ ⁇ of the core-cladding interface. At a larger angle (incident angle), the light travels through the core 160 with total reflection at the core / cladding interface, and reaches the illumination light exit surface 144. As shown in FIG. 9, the illumination light angle phi ° cores in (, ⁇ 2 ° ⁇ .) - After traveling through the core 1 6 0 while being totally reflected at the clad surface, the incident angle gamma ° ( ⁇ 2 ° ⁇ ) reaches the illumination light exit surface 144. Incident angle ⁇ . Is represented by equation (5).
  • ⁇ ° ⁇ ° — a ° ⁇ ⁇ ⁇ ⁇ 0 °
  • Equation (6) is derived from Equations (3) and (5) for the relationship
  • the illumination light traveling in the core 160 is totally reflected.
  • the illumination light reaching the end face 1 65 b of the optical transmission line exits from the core 160 and enters the inside of the finger 6. can do.
  • the light incident on the finger 6 becomes scattered light inside the finger 6, and a part of the scattered light reaches the uneven pattern input surface 122.
  • the scattered light of the finger 6 After passing through the air layer between the concave and convex pattern input surface 122 and the core 160, the light enters the core 160.
  • the light incident on the core 160 in this manner is not totally reflected at the core-cladding interface, passes through the cladding 161, and is absorbed by the light absorber 162.
  • the detection light incident on the core 160 from the finger 6 at the portion where the convex part of the belly of the finger 6 contacts the uneven pattern input surface 122 of the uneven pattern input surface 122 is The light travels through the core 160 while undergoing total internal reflection, and reaches the convex pattern output surface 124.
  • FIG. 10 is a diagram illustrating a mode in which the detection light that has entered the detection region 12 from the finger 6 is guided by the optical transmission line in the detection region 12.
  • the end face 16 5 a of the optical transmission path contacts the end face of the optical transmission path in contact with air
  • the end face 16 5 b of the optical transmission path contacts the finger 6. 2 shows an end surface of an optical transmission line.
  • the scattered light inside the finger 6 passes through the air layer between the finger 6 and the end surface 1 65 a of the optical transmission path in the portion located in the concave portion of the belly of the finger 6. Then, the end face of the optical transmission line reaches 1 65 a.
  • the axis is the slant angle in the angle range shown in Expression (4) with respect to the end surface 165 a of the optical transmission line.
  • the light that has passed through the air layer and entered the core 160 from the end face 16 a of the optical transmission line has a critical angle of ⁇ at the core-cladding interface. .
  • the angle of incidence At a smaller angle (the angle of incidence), it reaches the core-cladding interface and leaks into the cladding 161, without total internal reflection at the core-cladding interface.
  • Light that has passed through the clad 16 1 and reached the light absorber 16 2 is absorbed by the light absorber 16 2 and attenuated. Therefore, the light that has entered the portion of the concave / convex pattern input surface 122 located in the concave portion of the finger 6 (the end surface 165 a of the optical transmission path) does not reach the concave / convex pattern output surface 124.
  • the refractive index of the finger 6 is higher than the refractive index of the core 160 at the portion of the concave / convex pattern input surface 122 that comes into contact with the convex part of the belly of the finger 6, the angle of refraction is. There is no limit on the angle range of. ⁇ Therefore, the part of the detection light incident on the end face 1 65 b of the optical transmission line from the finger 6 is partly a critical angle 6 C at the core-cladding interface. At a larger angle (incident angle) than it reaches the core interface. This detection light travels through the core 160 while being totally reflected at the core-cladding interface, and reaches the uneven pattern output surface 124. Critical angle e c at the core-cladding interface of the detected light.
  • the light / dark pattern of the detection light corresponding to the concave / convex pattern of the antinode of the finger 6 is present on the convex pattern output surface 124. It is.
  • the convex pattern output surface 124 is joined to the light receiving surface 42 of the image sensor 4, and the image sensor 4 detects a light / dark pattern of detection light corresponding to the uneven pattern of the antinode of the finger 6.
  • the unevenness pattern detection device 2 is reduced in size and thickness. Also, the illumination light is guided to the illumination light exit surface 144 by the optical transmission path of the illumination area 14, and efficiently illuminates the finger 6 to be measured.
  • the refractive index n 2 of the clad in the illumination area 74 is lower than the refractive index of the clad in the fiber optical plate 1.
  • the structure of the fiber optical plate 7 is otherwise the same as the structure of the fiber optical plate 1.
  • FIG. 11 is a diagram showing a state in which the illumination light is emitted or reflected on the illumination light exit surface 744.
  • Part of the illuminating light guided by the optical transmission path in the illuminating region 74 has a critical angle of 6 C at the core-cladding interface of the fiber optic plate 1. At a smaller angle (incident angle), the light travels through the core with total reflection at the core / cladding interface, and reaches the illumination light exit surface 7444.
  • the illuminating light totally reflected at the core-cladding interface is the critical angle at the air-core interface] 3 c . Illumination at a smaller angle (incident angle) The light exit surface 744 is reached.
  • the illumination unit can more efficiently illuminate the measured object.
  • the refractive index ⁇ 3 of the core and the refractive index ⁇ 4 of the clad in the illumination area 84 are respectively the same as the refractive index ⁇ of the core in the fiber optical plate 1. .
  • the refractive index ⁇ of the cladding is otherwise the same as the structure of the fiber optical plate 1.
  • the refractive index ⁇ 3 of the core in the illumination region 84 is the refractive index of the core in the detection region 82 (the refractive index of the core in the fiber optic plate 1) ⁇ . Lower than. Therefore, in the illumination area 84, the critical angle at the air-core interface. Is larger than the critical angle at the air-core interface of the detection region 82 (the critical angle at the air ′ core interface of the fiber optic plate 1) c °. Further, the cladding refractive index n 4 of the illumination region 8 4, the illumination region 8 4 cores 'critical Sumo detection region 82 of the core at the cladding interface - critical angle at the cladding interface (fiber optics 1 Core' cladding the critical angle at the interface) 6 C. Is set to be equal to That is, the refractive index n 4 of the clad in the illumination region 8 4 is expressed by Equation (9).
  • n 4 n 3 -si ⁇ . . , ⁇ 3 ⁇ 0. (9)
  • FIG. 12 is a diagram showing a state in which the illumination light is emitted or reflected on the illumination light emission surface 844.
  • Illumination area 84 Core 'Illumination light that travels through the core while undergoing total reflection at the cladding interface has an incident angle of ⁇ . Reaches the illumination light emitting surface 844. Illumination area 8 4 core .cladding The critical angle at the interface is the critical angle e c at the core 'cladding interface of the fiber optic plate 1. Therefore, the relationship expressed by the above-described expression (6) is established even in the illumination area 84. That is, the following equation (10) is derived.
  • the illumination area 84 the air ⁇ critical angle at the core interface ⁇ . . But the critical angle 3 C in air ⁇ core interface of the fiber-optic plate 1. , The angle of incidence of some of the illumination light on the illumination light exit surface 84 4. Is the critical angle at the air-core interface in the illumination area 84. Smaller than. Such illumination light can also be emitted outside at a portion of the illumination light exit surface 844 that comes into contact with air. Therefore, the illumination means can more efficiently illuminate the measured object.
  • the interval at which the plurality of cores are arranged in the illumination area (the interval at which the center axis of the core is arranged) is set at the interval at which the plurality of cores are arranged at the detection area (the center axis of the core). It is preferable that the core area in the illumination area is larger than the core area in the detection area.
  • the thickness of the cladding of the optical fiber used to manufacture the multi-fiber (MF) or multi-multi-fiber (MM F) for the illumination area and the multi-fiber for the detection area is set at the interval at which the plurality of cores are arranged at the detection area (the center axis of the core).
  • the diameter of the core in the illumination area must be larger than the diameter of the core in the detection area, that is, the illumination area
  • the illumination direction of the LED array and the illumination area may be attached to the fiber optic plate so that the direction of the light transmission path matches.
  • FIG. 13 is a conceptual diagram showing a mode in which the LED array 20 is attached to the fiber optic plate 10.
  • the LED array 20 is arranged below the illumination light incident surface 1042 such that the illumination direction matches the direction of the light transmission path in the illumination area 104.
  • the LED array 20 and the illumination light incident surface 1042 are joined by the transparent resin 30.
  • the light receiving surface 40 is bonded to the concave / convex pattern output surface 1024 of the detection region 102.
  • FIG. 14 is a conceptual diagram showing a mode in which the LED array 60 is disposed below the illumination light incident surface 542 with the intermediate fiber optical plate 70 interposed therebetween. The same slant angle as the fiber optic plate 50 is set in the intermediate fiber optic plate 70.
  • an intermediate fiber optical plate 70 may be interposed between the concave / convex pattern output surface 524 and the light receiving surface 80.
  • FIG. 15 is a conceptual diagram showing a mode in which an intermediate fiber optical plate 70 is interposed between the LED array 60 and the light receiving surface 80 and the fiber optical plate 50.
  • FIG. 16 is a front view of the embedded LED array 9.
  • Figure 17 shows the XVII-XVII line of the embedded LED array 9 shown in Figure 16.
  • FIG. A plurality of embedding holes 906 for embedding the LEDs 904 are formed in the long board-shaped printed board 902 along the length direction of the printed board 902.
  • a bottom plate 908 constituting the bottom surface of the embedding hole 906 is attached to the printed circuit board 902 by soldering.
  • An LED 904 is installed on the bottom plate 908 and wired with lead wires 910.
  • the present invention is applicable to, for example, a fingerprint detector.

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  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)
  • Engineering & Computer Science (AREA)
  • Human Computer Interaction (AREA)
  • Multimedia (AREA)
  • Theoretical Computer Science (AREA)
  • Optical Fibers, Optical Fiber Cores, And Optical Fiber Bundles (AREA)
  • Optical Couplings Of Light Guides (AREA)
  • Length Measuring Devices By Optical Means (AREA)
  • Measurement Of The Respiration, Hearing Ability, Form, And Blood Characteristics Of Living Organisms (AREA)

Abstract

A fiber optical plate (1), comprising detection areas (12) where light absorbers are disposed around optical paths and illumination areas (14) where the light adsorber is not installed between the adjacent optical paths, wherein an irregular pattern output surface (124) and an imaging element (4) and an illumination light incident surface (142) and a LED array (5) are joined to each other with a transparent adhesive agent, whereby the axis of the optical paths and an irregular pattern input surface (122) are tilted at a slant angle set so that light incident from the air is not totally reflected on a core/clad boundary surface.

Description

明糸田書  Akitoda

ファイバ光学プレート及ぴ凹凸パターン検出装置  Fiber optic plate and uneven pattern detector

技術分野 Technical field

本発明は、 ファイバ光学プレート及びファイバ光学プレートが適用された凹凸 パターン検出装置に関するものである。  The present invention relates to a fiber optical plate and an uneven pattern detecting device to which the fiber optical plate is applied.

背景技術 Background art

近年、 カード型凹凸パターン (指紋) 検出装置の実現など、 認証装置の小型化 及び薄型化が求められている。かかる凹凸パターン検出装置を実現するためには、 被測定対象 (指) 内部の散乱光を利用して被測定対象表面の凹凸パターンを検出 する方法が適している。  In recent years, there has been a demand for a smaller and thinner authentication device, such as the realization of a card-shaped uneven pattern (fingerprint) detection device. In order to realize such a concavo-convex pattern detecting device, a method for detecting a concavo-convex pattern on the surface of the measurement target using scattered light inside the measurement target (finger) is suitable.

被測定対象内部の散乱光を利用した従来の凹凸パターン検出装置は、 例えば、 特許第 3045629号公報で開示されるように、 照明光が側方から被測定対象の内部 に入射した上、 被測定対象の内部で散乱した光が被側定対象の下方に配置される 凹凸パターン伝送手段に入射するものがあった。 また、 特開 2000- 217803号公報 で開示されるように、 受光素子の側方に配置される照明手段が、 受光素子の受光 面に置かれる被測定対象を照明するものがあった。  A conventional concavo-convex pattern detection device using scattered light inside the object to be measured is disclosed in, for example, Japanese Patent No. 3045629, in which illuminating light enters the inside of the object to be measured from the side, and In some cases, light scattered inside the target is incident on the concave / convex pattern transmission means arranged below the target object. Further, as disclosed in Japanese Patent Application Laid-Open No. 2000-217803, there has been an apparatus in which an illuminating unit arranged on a side of a light receiving element illuminates an object to be measured placed on a light receiving surface of the light receiving element.

発明の開示 , , . Disclosure of the invention,.

しかしながら、 特許第3045629号公報の凹凸パターン検出装置には、 凹凸パタ ーン伝送手段と分離された照明手段が、 被測定対象の側方、 すなわち検出面の斜 め上方に設置されるため、 装置の小型化又は薄型化に限界があるという問題があ つた。 また、 特開 2000-217803号公報の凹凸パターン検出装置には、 照明手段が 効率良く被測定対象を照明することができないという問題があった。 However, Japanese Patent No. 3 04 562 9 No. irregular pattern detector publications, for illuminating means which is separated from the concave-convex patterns transmission means, the side of the object to be measured, that is, disposed obliquely Me above the detection surface However, there is a problem in that the size or thickness of the device is limited. Further, the uneven pattern detection device disclosed in Japanese Patent Application Laid-Open No. 2000-217803 has a problem that the illumination means cannot efficiently illuminate the object to be measured.

本発明は、 上記問題を解決するためになされたものであり、 被測定対象内部の 散乱光を利用する凹凸パターン検出装置において装置が小型化又は薄型化される こと及び照明手段が効率良く被測定対象を照明することを可能ならしめるフアイ バ光学プレート及びファイバ光学プレートが適用された凹凸パターン検出装置を 提供することを目的とする。 SUMMARY OF THE INVENTION The present invention has been made to solve the above-described problems. In an uneven pattern detection device using scattered light inside an object to be measured, the device is reduced in size or thickness, and illumination means is efficiently measured. A fiber optic plate and a fiber optic plate that can illuminate an object The purpose is to provide.

上記目的を達成するために、 本発明のファイバ光学プレートは、 被測定対象の 凹凸パターンを検出する凹凸パターン検出装置に適用され、 各々の軸線が双方の 端面と斜めに交わり、クラッド中に複数のコアが所定の間隔で配置されるように、 複数の光ファイバを集成し、 成形したファイバ光学プレートであって、 凹凸パタ 一ンを撮像する撮像手段が臨む検出領域と、 検出領域に隣接すると共に、 被測定 対象を照明する照明手段が臨む照明領域と、 を含んで構成され、 検出領域におけ るクラッド中に、 光を吸収する光吸収体が設けられたことを特徴とする。  In order to achieve the above object, a fiber optical plate of the present invention is applied to an uneven pattern detecting device for detecting an uneven pattern of a measured object, and each axis crosses both end surfaces obliquely, and a plurality of fibers are formed in a clad. A plurality of optical fibers are aggregated and arranged so that the cores are arranged at predetermined intervals. The molded optical fiber plate is a fiber optical plate, and a detection area facing an imaging means for imaging an uneven pattern is provided. And an illumination area facing illumination means for illuminating the object to be measured, and a light absorber for absorbing light is provided in the cladding in the detection area.

凹凸パターン伝送手段として機能する検出領域では、 クラッド中に光吸収体が 設けられることにより、 被測定対象の凹凸パターンが撮像手段に高い精度で伝送 される。 他方、 照明領域では、 クラッド中に光吸収体が設けられないので、 照明 手段の発する照明光が被測定対象に効率良く導光される。 また、 本発明のフアイ バ光学プレートがかかる照明領域を備えることにより、 凹凸パターン検出装置を 作製する上で、 ファイバ光学プレートの照明光入射面に照明手段を取り付けて装 置を小型化又は薄型化させることが可能になる。  In the detection region functioning as the uneven pattern transmission means, the light absorber is provided in the clad, so that the uneven pattern of the measured object is transmitted to the imaging means with high accuracy. On the other hand, in the illumination area, since no light absorber is provided in the cladding, the illumination light emitted by the illumination means is efficiently guided to the object to be measured. In addition, since the fiber optical plate of the present invention is provided with such an illumination area, in manufacturing an uneven pattern detection device, an illumination means is attached to the illumination light incident surface of the fiber optical plate to reduce the size or thickness of the device. It becomes possible to do.

本発明のファイバ光学プレートは、 照明領域におけるクラッドの屈折率が、 検 出領域におけるクラ'ッドの屈折率よりも低いことが好適である.。 - . '.. 空気中の外乱光がコアに入射してもコア'クラッド界面で全反射しないように、 軸線がファイバ光学プレートの表面と所定の角度 (スラント角) で斜めに交わる ファイバ光学プレートにより導光される光は、 出射面のうち空気よりも屈折率の 高い物体が接触している部分においてのみ出射することができる。 しカゝし、 照明 領域におけるクラッドの屈折率を、 検出領域におけるクラッドの屈折率よりも低 くすることで、 照明領域におけるコア ·クラッド界面での臨界角が小さくなる。 そのため、 空気中の外乱光が検出領域において導光されないように、 スラント角 が設定されているファイバ光学プレートであっても、 照明領域では、 小さい角度 (入射角) でコア 'クラッド界面を全反射しつつコアの中を進行する照明光が、 出射面のうち空気と接触している部分においても、外部に出射できるようになる。 その結果、 被測定対象がより効率的に照明される。 In the fiber optical plate of the present invention, it is preferable that the refractive index of the cladding in the illumination region is lower than the refractive index of the cladding in the detection region. -'.. Fiber optic plate whose axis obliquely intersects the surface of the fiber optic plate at a predetermined angle (slant angle) so that even if disturbance light in the air enters the core, it will not be totally reflected at the core' cladding interface. Can be emitted only at a portion of the exit surface where an object having a higher refractive index than air is in contact. However, by making the refractive index of the cladding in the illumination region lower than the refractive index of the cladding in the detection region, the critical angle at the core-cladding interface in the illumination region becomes smaller. Therefore, even in the case of a fiber optic plate with a slant angle set so that disturbance light in the air is not guided in the detection area, in the illumination area, total reflection is performed at the core / cladding interface at a small angle (incident angle). The illumination light traveling through the core while The light can be emitted to the outside even at the part of the emission surface that is in contact with the air. As a result, the measured object is illuminated more efficiently.

本発明のファイバ光学プレートは、 照明領域におけるコアの屈折率が、 検出領 域におけるコアの屈折率よりも低いことが好適である。  In the fiber optic plate of the present invention, the refractive index of the core in the illumination region is preferably lower than the refractive index of the core in the detection region.

照明領域におけるコアの屈折率を、 検出領域におけるコアの屈折率よりも低く することにより、 照明領域における空気■コア界面での臨界角が大きくなる。 そ のため、 軸線と出射面とが斜めに交わるファイバ光学プレートであっても、 照明 領域では、 照明光が、 出射面のうち空気と接触している部分においても、 外部に 出射しやすくなる。 その結果、 被測定対象がより効率的に照明される。  By making the refractive index of the core in the illumination region lower than the refractive index of the core in the detection region, the critical angle at the air-core interface in the illumination region increases. Therefore, even in the case of a fiber optical plate in which the axis line and the emission surface obliquely intersect, in the illumination area, the illumination light is easily emitted to the outside even in the portion of the emission surface that is in contact with air. As a result, the measured object is illuminated more efficiently.

本発明のファイバ光学プレートは、 照明領域において複数のコアが配置される 間隔が、 検出領域において複数のコアが配置される間隔よりも長いことが好適で める。  In the fiber optic plate of the present invention, it is preferable that the interval at which the plurality of cores are arranged in the illumination area is longer than the interval at which the plurality of cores are arranged in the detection area.

照明領域において複数のコアが配置される間隔を、 検出領域におレ、て複数のコ ァが配置される間隔よりも長くすることにより、 コア間に介在するクラッドの厚 さを変えずに、 照明光の入射面におけるコアの面積割合を高くすることができ、 照明領域における照明光の入射効率が向上する。 他方、 検出領域において複数の コァが配置される間隔を相対的に短くすることで、 検出領域の表面における単位 面積当たりのコアの本数が多くなり、 検出領域において伝送される凹凸パターン の精度が向上する。  By making the interval at which a plurality of cores are arranged in the illumination area longer than the interval at which a plurality of cores are arranged in the detection area, the thickness of the clad interposed between the cores is not changed. The area ratio of the core on the incident surface of the illumination light can be increased, and the incidence efficiency of the illumination light on the illumination region is improved. On the other hand, by relatively shortening the interval at which multiple cores are arranged in the detection area, the number of cores per unit area on the surface of the detection area increases, and the accuracy of the concavo-convex pattern transmitted in the detection area improves. I do.

本発明の凹凸パターン検出装置は、 上記ファイバ光学プレートのうちのいずれ か一つを備え、 撮像手段が検出領域の一方の表面を臨むように取り付けられ、 照 明手段が照明領域の撮像手段が配置される側の表面を臨むように取り付けられる ことを特徴とする。  The uneven pattern detection device of the present invention includes any one of the fiber optical plates, wherein the imaging means is mounted so as to face one surface of the detection area, and the illumination means is arranged with the imaging means of the illumination area. It is attached so as to face the surface on the side to be cut.

本発明の凹凸パターン検出装置が上記ファイバ光学プレートを備えることによ り、 効率の良い被測定対象の照明を実現でき、 また照明領域の照明光入射面に照 明手段を取り付けることにより、 装置が小型化又は薄型化される。 図面の簡単な説明 Since the uneven pattern detection device of the present invention includes the above-described fiber optical plate, efficient illumination of the object to be measured can be realized, and the device can be mounted by attaching illumination means to the illumination light incident surface in the illumination area. The size or thickness is reduced. BRIEF DESCRIPTION OF THE FIGURES

図 1は、 ファイバ光学プレート 1が適用された凹凸パターン検出装置 2の平面 図である。  FIG. 1 is a plan view of an uneven pattern detecting device 2 to which a fiber optical plate 1 is applied.

図 2は、 図 1に示す凹凸パターン検出装置 2の II一 II線断面図である。  FIG. 2 is a cross-sectional view taken along the line II-II of the uneven pattern detecting device 2 shown in FIG.

図 3は、 図 1に示す凹凸パターン検出装置 2の III一 III線断面図である。 図 4は、 L E Dアレー 5の正面図である。  FIG. 3 is a sectional view taken along the line III-III of the uneven pattern detecting device 2 shown in FIG. FIG. 4 is a front view of the LED array 5.

図 5は、 図 4に示す L E Dアレー 5の V—V線に沿った断面図である。  FIG. 5 is a cross-sectional view of the LED array 5 shown in FIG. 4 along the line VV.

図 6は、 図 1に示すファイバ光学プレート 1の正面図である。  FIG. 6 is a front view of the fiber optic plate 1 shown in FIG.

図 7は、 検出領域 1 2におけるファイバ光学プレート 1の部分拡大断面図であ る。  FIG. 7 is a partially enlarged cross-sectional view of the fiber optic plate 1 in the detection area 12.

図 8は、 ファイバ光学プレート 1の上に被測定対象である指 6が置かれた状態 を示す図である。  FIG. 8 is a diagram showing a state where a finger 6 to be measured is placed on the fiber optical plate 1.

図 9は、 照明光出射面 1 4 4において、 照明光が出射又は反射する態様を示す 図である。  FIG. 9 is a view showing a mode in which the illumination light is emitted or reflected on the illumination light exit surface 144. As shown in FIG.

図 1 0は、 指 6から検出領域 1 2に入射した検出光が、 検出領域 1 2の光伝送 路によって導光される態様を示す図である。  FIG. 10 is a diagram illustrating a mode in which the detection light that has entered the detection region 12 from the finger 6 is guided by the optical transmission line in the detection region 12.

図 1 1は、 照明光出射面 7 4 4において、 照明光が出射又は反射する態様を示 す図である。  FIG. 11 is a diagram showing a state in which the illumination light is emitted or reflected on the illumination light exit surface 744.

図 1 2は、 照明光出射面 8 4 4において、 照明光が出射又は反射する態様を示 す図である。  FIG. 12 is a diagram illustrating a mode in which the illumination light is emitted or reflected on the illumination light emission surface 844.

図 1 3は、 ファイバ光学プレート 1 0に L E Dアレー 2 0が取り付けられる態 様を示す概念図である。  FIG. 13 is a conceptual diagram showing a state in which the LED array 20 is attached to the fiber optical plate 10.

図 1 4は、 L E Dアレー 6 0力 中間ファイバ光学プレート 7 0を挟んで、 照 明光入射面 5 4 2の下方に配置される態様を示す概念図である。  FIG. 14 is a conceptual diagram showing a mode in which the LED array 60 and the intermediate fiber optical plate 70 are disposed below the illumination light incidence surface 542 with the intermediate fiber optical plate 70 interposed therebetween.

図 1 5は、 L E Dアレー 6 0及び受光面 8 0とファイバ光学プレート 5 0との 間に中間ファイバ光学プレート 7 0が介在する態様を示す概念図である。 図 1 6は、 埋め込み型 L E Dアレー 9の正面図である。 FIG. 15 is a conceptual diagram showing a mode in which an intermediate fiber optical plate 70 is interposed between the LED array 60 and the light receiving surface 80 and the fiber optical plate 50. FIG. 16 is a front view of the embedded LED array 9.

図 1 7は、図 1 3に示す埋め込み型 L E Dアレー 9の XIV— XIV線に沿った断面 図である。  FIG. 17 is a cross-sectional view of the embedded LED array 9 shown in FIG. 13 taken along the line XIV-XIV.

発明を実施するための最良の形態 BEST MODE FOR CARRYING OUT THE INVENTION

以下、 添付図面を参照して、 本発明のファイバ光学プレート及びファイバ光学 プレートが適用された凹凸パターン検出装置の好適な実施形態について詳細に説 明する。  Hereinafter, preferred embodiments of a fiber optical plate and an uneven pattern detection device to which the fiber optical plate according to the present invention is applied will be described in detail with reference to the accompanying drawings.

[第 1実施形態]  [First Embodiment]

本発明の第 1の実施形態に係るフアイバ光学プレート 1及びファィバ光学プレ ート 1が適用された凹凸パターン検出装置 2の構造を説明する。  The structure of the fiber optical plate 1 and the uneven pattern detecting device 2 to which the fiber optical plate 1 according to the first embodiment of the present invention is applied will be described.

図 1は、 ファイバ光学プレート 1が適用された凹凸パターン検出装置 2の平面 図である。図 2は、図 1に示す凹凸パターン検出装置 2の II— II線断面図である。 図 3は、 図 1に示す凹凸パターン検出装置 2の III— III線断面図である。 枠体 3 は、 長方形の底面 3 2を備え、 底面 3 2の短手方向外側の対向する二辺にワイヤ 端子 3 4を 4個ずつ備える。 底面 3 2上の中央部に撮像素子 4が設置される。 撮 像素子 4は平板形状であり、 撮像素子 4の上面 (以下では、 底面 3 2から見て撮 像素子 4が設置される方向を上、その逆方向を下とする。).の中央部に長方形の受 光面 4 2を備え、撮像素子 4の上面のうち受光面 4 2の周囲に外枠 4 4を備える。 撮像素子 4の厚さは、 後述する L E Dアレー 5の厚さと一致する。 ここで、 撮像 素子 4は、 受光面 4 2の長手方向と、 底面 3 2の長手方向とがー致するように設 置される。 図 2及び図 3では、 撮像素子 4の表面のうち受光面 4 2に該当する部 分を太線で示す。 撮像素子 4は、 受光面 4 2の短手方向外側の対向する二辺 (外 枠 4 4上) にワイヤ端子 4 6を 4個ずつ備える。 ワイヤ端子 4 6と枠体 3のワイ ャ端子 3 4とがボンディングワイヤ 3 6で接続されることにより、 撮像素子 4が 配線される。  FIG. 1 is a plan view of an uneven pattern detecting device 2 to which a fiber optical plate 1 is applied. FIG. 2 is a cross-sectional view taken along the line II-II of the uneven pattern detecting device 2 shown in FIG. FIG. 3 is a sectional view taken along line III-III of the uneven pattern detection device 2 shown in FIG. The frame 3 has a rectangular bottom surface 32, and four wire terminals 34 on two opposite sides of the bottom surface 32 in the short side direction. The image sensor 4 is installed at the center on the bottom surface 32. The imaging device 4 has a flat plate shape, and the upper portion of the imaging device 4 (hereinafter, the direction in which the imaging device 4 is installed as viewed from the bottom surface 32 is the upper direction, and the opposite direction is the lower portion). The image sensor 4 has a rectangular light receiving surface 42, and an outer frame 44 around the light receiving surface 42 on the upper surface of the image sensor 4. The thickness of the imaging element 4 matches the thickness of the LED array 5 described later. Here, the image pickup device 4 is disposed such that the longitudinal direction of the light receiving surface 42 and the longitudinal direction of the bottom surface 32 match. 2 and 3, a portion corresponding to the light receiving surface 42 of the surface of the image sensor 4 is indicated by a thick line. The image sensor 4 includes four wire terminals 46 on two opposing sides (on the outer frame 44) of the light receiving surface 42 on the outer side in the lateral direction. The image sensor 4 is wired by connecting the wire terminals 46 and the wire terminals 34 of the frame 3 with bonding wires 36.

枠体 3の底面 3 2上の長手方向の対向する二辺に、 撮像素子 4と隣接するよう に、 L E Dアレー 5が設置される。 照明手段として機能する L E Dアレー 5は薄 い長板形状であり、 かかる薄板状の照明手段を適用することにより凹凸パターン 検出装置 2を薄型化することが可能となる。 L E Dアレー 5は、 長さ方向が底面 3 2の短手方向と一致するように設置される。 図 4は、 L E Dアレー 5の正面図 である。 図 5は、 図 4に示す L E Dアレー 5の V—V線に沿った断面図である。 L E Dアレー 5は、 底面に長板形状のプリント基板 5 0 2を備える。 プリント基板 5 0 2の上に、 プリント基板 5 0 2の長さ方向に沿って、 複数の L E D 5 0 4力 S 配置され、 さらに端部に抵抗器 5 0 6が設置される。 L E D 5 0 4及び抵抗器 5 0 6は、 リード線 5 0 8で配線される。 L E D 5 0 4及び抵抗器 5 0 6が設置さ れたプリント基板 5 0 2の表面は、 全体がエポキシ系透明樹脂 5 1 0で被覆され る。 The bottom surface 3 2 of the frame 3 should be adjacent to the image sensor 4 on two opposite sides in the longitudinal direction. LED array 5 is installed. The LED array 5 functioning as an illuminating means has a thin long plate shape, and by applying such a thin illuminating means, the uneven pattern detecting device 2 can be made thin. The LED array 5 is installed such that the length direction coincides with the short direction of the bottom surface 32. FIG. 4 is a front view of the LED array 5. FIG. 5 is a cross-sectional view of the LED array 5 shown in FIG. 4 along the line VV. The LED array 5 includes a long printed board 502 on the bottom surface. A plurality of LEDs 504 are arranged on the printed circuit board 502 along the longitudinal direction of the printed circuit board 502, and a resistor 506 is provided at the end. LED 504 and resistor 506 are wired with lead 508. The entire surface of the printed circuit board 502 on which the LED 504 and the resistor 506 are installed is covered with an epoxy-based transparent resin 510.

撮像素子 4及び L E Dアレー 5の上にファイバ光学プレート 1が設置される。 ファイバ光学プレート 1の表面は長方形であり、 その短手方向の長さが、 L E D アレー 5の長手方向の長さと一致し、 撮像素子 4の受光面 4 2の短手方向の長さ よりも長い。 ファイバ光学プレート 1は、 その表面の長手方向と枠体 3の底面 3 2の長手方向と一致し、 かつその表面が L E Dアレー 5の上面全体及び撮像素子 4の受光面 4 2全体を覆い、 ワイヤ端子 4 6とは接触し,な,いように設置される。 図 3に示すように、 ファイバ光学プレート 1は、 複数の光ファイバが各々の軸線 が平行となるように束ねられて一体的に集成されたものであり、 クラ,ッド中に複 数のコアが所定の間隔で配置される構造を有する。 また、 ファイバ光学プレート 1は、 軸線 (中心軸) とファイバ光学プレート 1の表面 (端面) とが、 角度 (ス ラント角) α °で、斜めに交わるようにスライスされる。 本実施形態ではファイバ 光学プレート 1の両端面は平行になっている。 ファイバ光学プレート 1は、 その 表面の長手方向の中央部に、 クラッド中に光吸収体が配置される検出領域 1 2を 備え、 両端部に、 クラッド中に光吸収体が配置されない照明領域 1 4を備える。 図 3では、 フアイバ光学プレート 1のうち検出領域 1 2に該当する部分を二重斜 線で、 照明領域 1 4に該当する部分を単斜線で示す。 検出領域 1 2の上面には、 被測定対象内部の散乱光を取り入れる凹凸パターン入力面 1 2 2が形成され、 検 出領域 1 2の下面には、 導光された散乱光 (検出光) が出射する凹凸パターン出 力面 1 2 4が形成される。 照明領域 1 4の下面には、 照明手段の発する照明光が 入射する照明光入射面 1 4 2が形成され、 照明領域 1 4の上面には、 導光された 照明光が出射する照明光出射面 1 4 4が形成される。 The fiber optic plate 1 is set on the image sensor 4 and the LED array 5. The surface of the fiber optic plate 1 is rectangular and its length in the short direction matches the length in the long direction of the LED array 5 and is longer than the length in the short direction of the light receiving surface 42 of the image sensor 4 . The fiber optical plate 1 coincides with the longitudinal direction of its surface and the longitudinal direction of the bottom surface 32 of the frame 3, and its surface covers the entire upper surface of the LED array 5 and the entire light receiving surface 42 of the image sensor 4. The terminal 46 is in contact with the terminal 46 and is not installed. As shown in FIG. 3, the fiber optic plate 1 is composed of a plurality of optical fibers bundled together so that their axes are parallel to each other, and a plurality of cores in a clad. Are arranged at predetermined intervals. The fiber optical plate 1 is sliced so that the axis (center axis) and the surface (end face) of the fiber optical plate 1 obliquely intersect at an angle (slant angle) α °. In the present embodiment, both end faces of the fiber optical plate 1 are parallel. The fiber optic plate 1 has a detection area 12 in the center of the surface in the longitudinal direction where the light absorber is arranged in the clad, and an illumination area 14 in which the light absorber is not arranged in the clad at both ends. Is provided. In FIG. 3, the portion of the fiber optical plate 1 corresponding to the detection area 12 is double oblique. The portion corresponding to the illumination area 14 is indicated by a solid line. On the upper surface of the detection area 12, an uneven pattern input surface 122 for taking in the scattered light inside the object to be measured is formed, and on the lower surface of the detection area 12, the scattered light (detection light) guided is provided. A projection pattern output surface 124 to be emitted is formed. On the lower surface of the illumination area 14, there is formed an illumination light entrance surface 142 on which the illumination light emitted by the illumination means is incident, and on the upper surface of the illumination area 14, the illumination light emission from which the guided illumination light exits Surfaces 144 are formed.

図 6は、 図 1に示すファイバ光学プレート 1の正面図である。 図 6の点を付し た領域がファイバ光学プレート 1の表面のうち凹凸パターン入力面 1 2 2を示し、 点を付した領域以外の部分が照明光出射面 1 4 4を示す。  FIG. 6 is a front view of the fiber optic plate 1 shown in FIG. The dotted area in FIG. 6 indicates the concave / convex pattern input surface 122 of the surface of the fiber optical plate 1, and the portion other than the dotted area indicates the illumination light emitting surface 144.

ファイバ光学プレート 1は、 撮像素子 4の受光面 4 2全体が凹凸パターン出力 面 1 2 4と接触し、かつ L E Dアレー 5が照明光入射面 1 4 2と接触するように、 設置される。 ファイバ光学プレート 1と撮像素子 4及び L E Dアレー 5とは透明 接着剤 (エポキシ系又はシリコーン系樹脂) で接合される。  The fiber optical plate 1 is installed such that the entire light receiving surface 42 of the image sensor 4 contacts the concave / convex pattern output surface 124, and the LED array 5 contacts the illumination light incident surface 142. The fiber optic plate 1 and the image sensor 4 and the LED array 5 are joined with a transparent adhesive (epoxy or silicone resin).

図 7は、 検出領域 1 2におけるファイバ光学プレート 1の部分拡大断面図であ る。 各光伝送路 (以下、 ファイバ光学プレート 1のうち、 コア及び当該コアを包 囲するクラッドによって構成される部分を 「光伝送路」 という。) は、 コア 1 6 0 を中心に有し、 ク.ラッド 1 6 1がコア 1 6 0を密着包囲する。 さらに、 光吸収体 1 6 2がクラッド 1 6 1を密着包囲する。 各光伝送路の両端面 1 6 5は、 軸線 1 6 4に対して角度 (スラント角) ひ。で傾斜する。 このスラント角 。は、 空気中 からコア 1 6 0に光が入射しても、 コア 1 6 0とクラッド 1 6 1との境界面で入 射光が全反射しないような角度に設定される。 すなわち、 所定のスラント角ひ。 の下では、 空気中からコア 1 6 0に入射する光は、 光伝送路の端面 1 6 5を通過 する際、 屈折角 /3 °において空気■コア界面で屈折し、 その後、 コア 'クラッド界 面における臨界角よりも小さい角度 (入射角) でコア■クラッド界面に達する。 スラント角 α。は、 特定の角度ひ c。を用いて、 ひ。≤ ひ。。と表すことができる。 こ こで、 a c°、 次の式(1)ないし(3)を満足する角度である。 ただし、 n。はコア 1 6 0の屈折率、 ηιはクラッド 1 6 1の屈折率、 naは空気の屈折率である。また、 6C° はコア ·クラッド界面における臨界角、 。。は空気中から光伝送路の端面 1 6 5 に入射角略 9 0°で入射した光の屈折角である。 FIG. 7 is a partially enlarged cross-sectional view of the fiber optic plate 1 in the detection area 12. Each optical transmission line (hereinafter, a portion of the fiber optical plate 1 that is constituted by a core and a clad surrounding the core is referred to as an “optical transmission line”) has a core 160 as a center, and Rad 16 1 closely surrounds core 160. Further, the light absorber 16 2 closely surrounds the clad 16 1. Both ends 16 5 of each optical transmission line are angled (slant angle) with respect to axis 16 4. Incline. This slant angle. The angle is set such that, even when light enters the core 160 from the air, the incident light is not totally reflected at the interface between the core 160 and the clad 161. That is, a predetermined slant angle. Below, the light incident on the core 160 from the air is refracted at the air / core interface at a refraction angle of 3 ° when passing through the end face 1650 of the optical transmission line, and then the core's cladding boundary It reaches the core-cladding interface at an angle (incident angle) smaller than the critical angle on the surface. Slant angle α. The specific angle c . By using ≤ h. . It can be expressed as. Here, ac ° is an angle that satisfies the following equations (1) to (3). Where n. Is core 1 6 Refractive index of 0, ηι the refractive index of the cladding 1 6 1, n a is the refractive index of air. 6 C ° is the critical angle at the core-cladding interface. . Is the refraction angle of the light incident from the air to the end face 1 65 of the optical transmission line at an incident angle of about 90 °.

n0 - s i ηθ。°= η s i n 9 0 ° (コア 'クラッド界面における屈折の法則) ··· (1) n 0 -si ηθ. ° = η sin 90 ° (core's law of refraction at the clad interface) ··· (1)

η0 · s i n ^c°= na · s i n 9 0。(空気'コア界面における屈折の法則) · · ·(2) a0°+ (i30°+ 9 0°) + (9 0°— 6C°) = 1 8 0°··· (3) η 0 · sin ^ c ° = n a · sin 90. (The law of refraction at the air-core interface) · · (2) a 0 ° + (i3 0 ° + 90 °) + (90 °-6 ° C ) = 180 ° (3)

式(1)ないし(3)から求まる o;c。を考慮すると、 上記のスラント角 ο;。の範囲 は、 式 (4)で表される。 O; c obtained from equations (1) to (3). Considering the above slant angle ο; Is expressed by equation (4).

°≤ a

Figure imgf000010_0001
n0) 一 s i n"1 、 n &/ n。リ · · · (4) ° ≤ a
Figure imgf000010_0001
n 0 ) one sin " 1 , n & / n. (4)

照明領域 1 4においては、 隣り合う光伝送路の間に光吸収体が介在しない。 照 明領域 1 4の光伝送路を構成するコア及びクラッドは、 検出領域 1 2の光伝送路 を構成するコア 1 6 0及びクラッド 1 6 1と同質のものである。  In the illumination area 14, no light absorber intervenes between adjacent light transmission paths. The core and the clad constituting the optical transmission line of the illumination region 14 are of the same quality as the core 160 and the cladding 161 constituting the optical transmission line of the detection region 12.

次に、 ファイバ光学プレート 1の製造方法を説明する。  Next, a method for manufacturing the fiber optical plate 1 will be described.

クラッドが光吸収体で被覆される光ファイバを集成することにより、 マルチフ アイバ (MF) 又はマルチマルチファイバ (MMF) 検出領域用に製造され る。また、クラッドが光吸収体で被覆されない光ファイバを集成することにより、 - マルチファイバ (MF) 又はマルチマルチファイバ (MMF) 力 照明領域用に 製造される。 ただし、 検出領域用のマルチファイバ (MF) 又はマルチマルチフ アイバ (MMF) の製造に用いられる光ファイバと、 照明領域用のマルチフアイ バ (MF) 又はマルチマルチファイバ (MMF) の製造に用いられる光ファイノ とは、 同一の外径とする。 検出領域用のマルチファイバ (MF) 又はマルチマル チファイバ (MMF) と、 照明領域用のマルチファイバ (MF) 又はマルチマル チファイバ (MMF) とが必要な高さだけ金型に整列される。 この際、 検出領域 用のマルチファイバ (MF) 又はマルチマルチファイバ (MMF) の製造に用い られる光ファイバと、 照明領域用のマルチファイバ (MF) 又はマルチマルチフ アイバ (MM F ) の製造に用いられる光ファイバとの外径とが同一であるので、 境界面での乱れがなくなる。 Fabricated for multi-fiber (MF) or multi-multi-fiber (MMF) sensing areas by assembling an optical fiber whose cladding is coated with a light absorber. Also, by assembling an optical fiber whose cladding is not covered with a light absorber,-Multi-fiber (MF) or Multi-multi-fiber (MMF) is manufactured for the illumination area. However, the optical fiber used to manufacture the multi-fiber (MF) or multi-multi-fiber (MMF) for the detection area and the optical fiber used to manufacture the multi-fiber (MF) or multi-multi-fiber (MMF) for the illumination area Phino has the same outer diameter. The multi-fiber (MF) or multi-multi fiber (MMF) for the detection area and the multi-fiber (MF) or multi-multi fiber (MMF) for the illumination area are aligned in the mold by the required height. At this time, the optical fiber used to manufacture the multi-fiber (MF) or multi-multi fiber (MMF) for the detection area and the multi-fiber (MF) or multi-multi fiber for the illumination area Since the outer diameter of the optical fiber used in the manufacture of Aiva (MM F) is the same as that of the optical fiber, disturbance at the interface is eliminated.

整列されたマルチファイバ (M F ) 又はマルチマルチファイバ (MM F ) は、 加熱プレス工程で融着される。  The aligned multi-fiber (M F) or multi-multi-fiber (MM F) is fused in a hot pressing process.

融着体がスライス '研磨されることにより、 ファイバ光学プレート 1が完成す る。  The fiber optic plate 1 is completed by slicing and polishing the fused body.

次に、 凹凸パターン検出装置 2が被測定対象表面の凹凸パターンを検出する動 作を説明する。  Next, an operation in which the uneven pattern detecting device 2 detects the uneven pattern on the surface of the measured object will be described.

図 8は、 ファイバ光学プレート 1の上に被測定対象である指 6が置かれた状態 を示す図である。 図 8に示すように、 指 6は、 指 6の腹が凹凸パターン入力面 1 2 2及び照明光出射面 1 4 4を覆うように、 ファイバ光学プレート 1の上に置か れる。  FIG. 8 is a diagram showing a state where a finger 6 to be measured is placed on the fiber optical plate 1. As shown in FIG. 8, the finger 6 is placed on the fiber optical plate 1 such that the belly of the finger 6 covers the uneven pattern input surface 122 and the illumination light emission surface 144.

L E Dアレー 5が発する照明光は、 照明光入射面 1 4 2から照明領域 1 4に入 射する。 照明領域 1 4に入射した照明光は、 照明領域 1 4の光伝送路によって導 光され、 照明光出射面 1 4 4に達する。 照明光出射面 1 4 4に達した照明光は、 照明光出射面 1 4 4のうち指 6の腹の凸部と接触する部分において、 指 6の内部 に入射して散乱光になる。 他方、 照明光出射面 1' 4 4に達した照明光は、 照明光 出射面 1 4 4のうち指 6の腹の凹部に位置する部分、 すなわち空気と照明光出射 面 1 4 4とが接する部分においては、 照明光出射面 1 4 4で全反射する。  The illumination light emitted from the LED array 5 enters the illumination area 14 from the illumination light incident surface 14 2. The illumination light that has entered the illumination area 14 is guided by the optical transmission path of the illumination area 14 and reaches the illumination light exit surface 144. The illumination light that has reached the illumination light exit surface 144 enters the inside of the finger 6 at the portion of the illumination light exit surface 144 that contacts the convex part of the finger 6, and becomes scattered light. On the other hand, the illuminating light that has reached the illuminating light exit surface 1 '44 is a portion of the illuminating light exit surface 144 that is located in the concave portion of the belly of the finger 6, i.e., the air comes into contact with the illuminating light exit surface 144. In the portion, the light is totally reflected by the illumination light exit surface 144.

図 9は、 照明光出射面 1 4 4において、 照明光が出射又は反射する態様を示す 図である。 図 9に示す光伝送路の端面 1 6 5 aは、 空気と接する光伝送路の端面 を示し、 光伝送路の端面 1 6 5 bは、 指 6と接する光伝送路の端面を示す。  FIG. 9 is a view showing a mode in which the illumination light is emitted or reflected on the illumination light exit surface 144. As shown in FIG. The end surface 165 a of the optical transmission line shown in FIG. 9 indicates the end surface of the optical transmission line in contact with air, and the end surface 165 b of the optical transmission line indicates the end surface of the optical transmission line in contact with the finger 6.

図 9を参照して、 照明光出射面 1 4 4において照明光が出射又は反射する過程 を詳細に説明する。照明領域 1 4の光伝送路によって導光される照明光は、コア - クラッド界面の臨界角 θε。よりも大きい角度 (入射角) においてコア 'クラッド 界面で全反射しながらコア 1 6 0の中を進行し、 照明光出射面 1 4 4に達する。 図 9に示すように、 照明光は、 角度 φ° ( 。、 Φ2°···) においてコア -クラッ ド界面で全反射しながらコア 1 6 0の中を進行した後、入射角 γ° (γΛ γ2°···) で照明光出射面 1 44に達する。 入射角 γ。は、 式 (5)で表される。 With reference to FIG. 9, a process of emitting or reflecting the illumination light on the illumination light exit surface 144 will be described in detail. The illumination light guided by the optical transmission path in the illumination area 14 has a critical angle θ ε of the core-cladding interface. At a larger angle (incident angle), the light travels through the core 160 with total reflection at the core / cladding interface, and reaches the illumination light exit surface 144. As shown in FIG. 9, the illumination light angle phi ° cores in (, Φ 2 ° ···.) - After traveling through the core 1 6 0 while being totally reflected at the clad surface, the incident angle gamma ° (γΛγ 2 ° ···) reaches the illumination light exit surface 144. Incident angle γ. Is represented by equation (5).

γ °= φ °— a ° φ ϋ0°· · · (5) γ ° = φ ° — a ° φ ϋ ^ θ 0 °

ここで、 入射角 y。と空気中から光伝送路の端面 1 6 5に入射角略 9 0°で入射 した光の屈折角 (空気 ·コア界面 (光伝送路の端面 1 6 5 a ) における臨界角) 3C°との関係について、 式(3)及び (5)より、 式 (6)が導かれる。 Where incident angle y. The angle of refraction of the light incident on the end face of the optical transmission line from the air at an incident angle of about 90 ° (the critical angle at the air-core interface (end face of the optical transmission path)) is 3 C °. Equation (6) is derived from Equations (3) and (5) for the relationship

β 0° = θ0°— α0°^θ0°—ひ。 φ。一(¾。 = γ。·· · (6) β 0 ° = θ 0 ° - α 0 ° ^ θ 0 ° - Fei. φ. One (¾. = Γ. · · · (6)

したがって、 光伝送路の端面 1 6 5 aにおいては、 コア 1 6 0の中を進行した 照明光は、 全反射する。  Therefore, on the end surface 1 65a of the optical transmission line, the illumination light traveling in the core 160 is totally reflected.

他方、 指 6の屈折率はコア 1 6 0の屈折率よりも高いので、 光伝送路の端面 1 6 5 bに達した照明光は、 コア 1 6 0から出射して指 6の内部へ入射することが できる。  On the other hand, since the index of refraction of the finger 6 is higher than the index of refraction of the core 160, the illumination light reaching the end face 1 65 b of the optical transmission line exits from the core 160 and enters the inside of the finger 6. can do.

指 6に入射した光は、 指 6内部の散乱光となり、 その一部が、 凹凸パターン入 力面 1 2 2に達する。 凹凸パターン入力面 1 2 2のうち指 6の腹の凹部に位置す る部分、 すなわち空気と凹凸パターン入力面 1 2 2とが接する部分においては、 '指 6內部の散乱光は、 指 6と凹凸パターン入力面 1 2 2との.間の空気層を通過し た後にコア 1 6 0に入射する。このようにしてコア 1 6 0に入射した光は、コア■ クラッド界面で全反射せず、 クラッド 1 6 1を透過した後、 光吸収体 1 6 2に吸 収される。 他方、 凹凸パターン入力面 1 2 2のうち指 6の腹の凸部と凹凸パター ン入力面 1 2 2とが接する部分において指 6からコア 1 6 0に入射した検出光は、 コア 'クラッド界面で全反射しながらコア 1 6 0の中を進行し、 囬凸パターン出 力面 1 2 4に達する。  The light incident on the finger 6 becomes scattered light inside the finger 6, and a part of the scattered light reaches the uneven pattern input surface 122. In the portion of the concave / convex pattern input surface 1 2 2 which is located in the concave portion of the belly of the finger 6, that is, in the portion where the air contacts the concave / convex pattern input surface 1 2 2, the scattered light of the finger 6 After passing through the air layer between the concave and convex pattern input surface 122 and the core 160, the light enters the core 160. The light incident on the core 160 in this manner is not totally reflected at the core-cladding interface, passes through the cladding 161, and is absorbed by the light absorber 162. On the other hand, the detection light incident on the core 160 from the finger 6 at the portion where the convex part of the belly of the finger 6 contacts the uneven pattern input surface 122 of the uneven pattern input surface 122 is The light travels through the core 160 while undergoing total internal reflection, and reaches the convex pattern output surface 124.

図 1 0は、 指 6から検出領域 1 2に入射した検出光が、 検出領域 1 2の光伝送 路によって導光される態様を示す図である。 図 9と同様、 光伝送路の端面 1 6 5 aは、 空気と接する光伝送路の端面を、 光伝送路の端面 1 6 5 bは、 指 6と接す る光伝送路の端面を示す。 FIG. 10 is a diagram illustrating a mode in which the detection light that has entered the detection region 12 from the finger 6 is guided by the optical transmission line in the detection region 12. As in FIG. 9, the end face 16 5 a of the optical transmission path contacts the end face of the optical transmission path in contact with air, and the end face 16 5 b of the optical transmission path contacts the finger 6. 2 shows an end surface of an optical transmission line.

図 1 0を参照して、 指 6から検出領域 1 2に入射した検出光が、 検出領域 1 2 の光伝送路によって導光される過程を詳細に説明する。  With reference to FIG. 10, the process in which the detection light that has entered the detection region 12 from the finger 6 is guided by the optical transmission line of the detection region 12 will be described in detail.

凹凸パターン入力面 1 2 2のうち指 6の腹の凹部に位置する部分においては、 指 6内部の散乱光は、 指 6と光伝送路の端面 1 6 5 aとの間の空気層を通過して 光伝送路の端面 1 6 5 aに達する。 前述のとおり、 検出領域 1 2の光伝送路にお いて、軸線は、光伝送路の端面 1 6 5 aに対し、式 (4)に示す角度範囲のスラント 角ひ。で傾斜しているので、空気層を通過して光伝送路の端面 1 6 5 aからコア 1 6 0に入射した光は、 コア ·クラッド界面における臨界角 Θ。。より小さい角度(入 射角) でコア 'クラッド界面に達することになり、 コア ·クラッド界面で全反射 せずに、 クラッド 1 6 1に漏出する。 クラッド 1 6 1を透過して光吸収体 1 6 2 に達した光は、 光吸収体 1 6 2に吸収されて減衰する。 そのため、 凹凸パターン 入力面 1 2 2のうち指 6の腹の凹部に位置する部分 (光伝送路の端面 1 6 5 a ) に入射した光は、 凹凸パターン出力面 1 2 4に到達しない。  In the concave / convex pattern input surface 1 2 2, the scattered light inside the finger 6 passes through the air layer between the finger 6 and the end surface 1 65 a of the optical transmission path in the portion located in the concave portion of the belly of the finger 6. Then, the end face of the optical transmission line reaches 1 65 a. As described above, in the optical transmission line of the detection region 12, the axis is the slant angle in the angle range shown in Expression (4) with respect to the end surface 165 a of the optical transmission line. The light that has passed through the air layer and entered the core 160 from the end face 16 a of the optical transmission line has a critical angle of 界面 at the core-cladding interface. . At a smaller angle (the angle of incidence), it reaches the core-cladding interface and leaks into the cladding 161, without total internal reflection at the core-cladding interface. Light that has passed through the clad 16 1 and reached the light absorber 16 2 is absorbed by the light absorber 16 2 and attenuated. Therefore, the light that has entered the portion of the concave / convex pattern input surface 122 located in the concave portion of the finger 6 (the end surface 165 a of the optical transmission path) does not reach the concave / convex pattern output surface 124.

凹凸パターン入力面 1 2 2のうち指 6の腹の凸部と接触する部分においては、 指 6の屈折率は、 コア 1 6 0の屈折率よりも高いので、屈折角 。の角度範囲に制 限はない。· したがって '指 6から光伝送路の端面 1 6 5 bに入射した検出光の.一 部は、 コア ·クラッド界面における臨界角 6C。よりも大きい角度 (入射角) でコ ァ 'クラッド界面に達する。 この検出光は、 コア -クラッド界面で全反射しなが らコア 1 6 0の中を進行し、 凹凸パターン出力面 1 2 4に達する。 検出光のうち コア ·クラッド界面における臨界角 ec。よりも小さい角度 (入射角) でコア -ク ラッド界面に達したものは、 クラッド 1 6 1に漏出する。 し力 し、 クラッド 1 6 1の周囲には光吸収体 1 6 1が配置されているので、 クラッド 1 6 1に漏出した 検出光が、 隣り合う光伝送路に漏出することはない。 Since the refractive index of the finger 6 is higher than the refractive index of the core 160 at the portion of the concave / convex pattern input surface 122 that comes into contact with the convex part of the belly of the finger 6, the angle of refraction is. There is no limit on the angle range of. · Therefore, the part of the detection light incident on the end face 1 65 b of the optical transmission line from the finger 6 is partly a critical angle 6 C at the core-cladding interface. At a larger angle (incident angle) than it reaches the core interface. This detection light travels through the core 160 while being totally reflected at the core-cladding interface, and reaches the uneven pattern output surface 124. Critical angle e c at the core-cladding interface of the detected light. Anything that reaches the core-cladding interface at a smaller angle (angle of incidence) leaks into the cladding 161. However, since the light absorber 161 is disposed around the clad 161, the detection light leaked to the clad 161 does not leak to the adjacent optical transmission line.

以上に述べた、 検出光を導光する検出領域 1 2の動作により、 囬凸パターン出 力面 1 2 4には、 指 6の腹の凹凸パターンに対応する検出光の明暗パターンが現 れる。 Due to the operation of the detection region 12 for guiding the detection light as described above, the light / dark pattern of the detection light corresponding to the concave / convex pattern of the antinode of the finger 6 is present on the convex pattern output surface 124. It is.

囬凸パターン出力面 1 2 4は撮像素子 4の受光面 4 2と接合されており、 指 6 の腹の凹凸パターンに対応する検出光の明暗パターンが撮像素子 4により検出さ れる。  囬 The convex pattern output surface 124 is joined to the light receiving surface 42 of the image sensor 4, and the image sensor 4 detects a light / dark pattern of detection light corresponding to the uneven pattern of the antinode of the finger 6.

本実施形態では、 照明光入射面 1 4 2に L E Dアレー 5を接合させることによ り、 凹凸パターン検出装置 2が小型化 ·薄型化される。 また、 照明光が、 照明領 域 1 4の光伝送路により照明光出射面 1 4 4に導光され、 効率良く被測定対象で ある指 6を照明する。  In the present embodiment, by joining the LED array 5 to the illumination light incidence surface 142, the unevenness pattern detection device 2 is reduced in size and thickness. Also, the illumination light is guided to the illumination light exit surface 144 by the optical transmission path of the illumination area 14, and efficiently illuminates the finger 6 to be measured.

[第 2実施形態]  [Second embodiment]

本発明の第 2の実施形態に係るファイバ光学プレート 7では、 照明領域 7 4に おけるクラッドの屈折率 n 2が、ファイバ光学プレート 1におけるクラッドの屈折 率 よりも低い。 ファイバ光学プレート 7の構造は、その他の点については、 フ アイバ光学プレート 1の構造と同じである。 In the fiber optical plate 7 according to the second embodiment of the present invention, the refractive index n 2 of the clad in the illumination area 74 is lower than the refractive index of the clad in the fiber optical plate 1. The structure of the fiber optical plate 7 is otherwise the same as the structure of the fiber optical plate 1.

照明領域 7 4におけるのクラッドの屈折率 η 2が、ファイバ光学プレート 1にお けるクラッドの屈折率 よりも低いので、 式(7)に示されるとおり、 照明領域 7 4では、 コア .クラッド界面における臨界角 。が、 ファイバ光学プレート 1の コア ·クラッド界面における臨界角 Θ。。よりも小さくなる。 Since the refractive index η 2 of the cladding in the illumination region 74 is lower than the refractive index of the cladding in the fiber optic plate 1, as shown in equation (7), in the illumination region 74, at the core-cladding interface, Critical angle. Is the critical angle at the core-cladding interface of the fiber optic plate 1. . Smaller than.

η0°= s i n "1 ( n 9 η 0) < θ0°= s i n—1 ( n x/ n 0) … (7) , η 0 ° = sin " 1 (n 9 η 0 ) <θ 0 ° = sin— 1 (n x / n 0 )… (7),

図 1 1は、 照明光出射面 7 4 4において、 照明光が出射又は反射する態様を示 す図である。  FIG. 11 is a diagram showing a state in which the illumination light is emitted or reflected on the illumination light exit surface 744.

照明領域 7 4の光伝送路により導光される照明光の一部は、 ファイバ光学プレ ート 1のコア ·クラッド界面における臨界角 6C。よりも小さい角度 (入射角) に おいてコア 'クラッド界面で全反射しながらコアの中を進行し、 照明光出射面 7 4 4に達する。 Part of the illuminating light guided by the optical transmission path in the illuminating region 74 has a critical angle of 6 C at the core-cladding interface of the fiber optic plate 1. At a smaller angle (incident angle), the light travels through the core with total reflection at the core / cladding interface, and reaches the illumination light exit surface 7444.

式 (8)を満たす角度 (入射角) η°においてコア ·クラッド界面で全反射した照 明光は、 空気■ コア界面における臨界角 ]3 c。よりも小さい角度 (入射角) で照明 光出射面 744に達する。At an angle satisfying the formula (8) (incident angle) η °, the illuminating light totally reflected at the core-cladding interface is the critical angle at the air-core interface] 3 c . Illumination at a smaller angle (incident angle) The light exit surface 744 is reached.

°≤;il。<6c。+ α °) · · · (8) ° ≤; il. < 6c . + α °)

したがって、 照明領域 74の光伝送路によって導光される照明光のうち式(8) を満たす角度 (入射角) においてコア 'クラッド界面で全反射するものは、 照 明光出射面 74 4のうち空気と接する部分においても外部に出射することができ る。そのため、照明手段が、 より効率的に、被測定対象を照明することができる。  Therefore, of the illumination light guided by the optical transmission path in the illumination area 74, the one that is totally reflected at the core / cladding interface at an angle (incident angle) that satisfies Equation (8) is the air out of the illumination light exit surface 744 The light can also be emitted to the outside even at the portion in contact with. Therefore, the illumination unit can more efficiently illuminate the measured object.

[第 3実施形態]  [Third embodiment]

本発明の第 3の実施形態に係るフアイバ光学プレート 8では、 照明領域 8 4に おけるコアの屈折率 η3及びクラッドの屈折率 η4が、 それぞれ、 ファイバ光学プ レート 1におけるコアの屈折率 η。及びクラッドの屈折率 ηιよりも低い。 フアイ バ光学プレート 8の構造は、 その他の点については、 ファイバ光学プレート 1の 構造と同じである。 In the fiber optical plate 8 according to the third embodiment of the present invention, the refractive index η 3 of the core and the refractive index η 4 of the clad in the illumination area 84 are respectively the same as the refractive index η of the core in the fiber optical plate 1. . And the refractive index ηι of the cladding. The structure of the fiber optical plate 8 is otherwise the same as the structure of the fiber optical plate 1.

照明領域 8 4におけるコアの屈折率 η3は、検出領域 8 2におけるコアの屈折率 (ファイバ光学プレート 1におけるコアの屈折率) η。よりも低い。 したがつ て、 照明領域 8 4では、 空気■コア界面における臨界角 。は、検出領域 8 2の空 気 - コア界面における臨界角 (ファイバ光学プレート 1の空気 'コア界面におけ る臨界角) c°よりも大きくなる。 また、 照明領域 8 4におけるクラッドの屈折 率 n4は、照明領域 8 4のコア'クラッド界面での臨界角力 検出領域 8 2のコア- クラッド界面での臨界角 (ファイバ光学プレート 1のコア 'クラッド界面での臨 界角) 6C。と等しくなるよう設定される。 すなわち、 照明領域 8 4におけるクラッ ドの屈折率 n4は式 (9)で表される。 The refractive index η 3 of the core in the illumination region 84 is the refractive index of the core in the detection region 82 (the refractive index of the core in the fiber optic plate 1) η. Lower than. Therefore, in the illumination area 84, the critical angle at the air-core interface. Is larger than the critical angle at the air-core interface of the detection region 82 (the critical angle at the air ′ core interface of the fiber optic plate 1) c °. Further, the cladding refractive index n 4 of the illumination region 8 4, the illumination region 8 4 cores 'critical Sumo detection region 82 of the core at the cladding interface - critical angle at the cladding interface (fiber optics 1 Core' cladding the critical angle at the interface) 6 C. Is set to be equal to That is, the refractive index n 4 of the clad in the illumination region 8 4 is expressed by Equation (9).

n4= n3 - s i ηθ。。、 η3< η0. ·· (9) n 4 = n 3 -si ηθ. . , Η 30. (9)

図 1 2は、 照明光出射面 8 44において、 照明光が出射又は反射する態様を示 す図である。  FIG. 12 is a diagram showing a state in which the illumination light is emitted or reflected on the illumination light emission surface 844.

照明領域 8 4のコア 'クラッド界面で全反射しながらコアの中を進行した照明 光は、 入射角 ζ。で照明光出射面 8 44に達する。 照明領域 8 4のコア .クラッド 界面における臨界角がファイバ光学プレート 1のコア 'クラッド界面における臨 界角 ec。と等しくなるよう設定されるので、 照明領域 8 4でも、 前述の式 (6)に示 される関係が成立する。 すなわち、 次の式(10)が導かれる。 Illumination area 84 Core 'Illumination light that travels through the core while undergoing total reflection at the cladding interface has an incident angle of ζ. Reaches the illumination light emitting surface 844. Illumination area 8 4 core .cladding The critical angle at the interface is the critical angle e c at the core 'cladding interface of the fiber optic plate 1. Therefore, the relationship expressed by the above-described expression (6) is established even in the illumination area 84. That is, the following equation (10) is derived.

β ο°≤ζ°. · · (10) β ο ° ≤ζ °. · (10)

しかし、 照明領域 8 4では、 空気■コア界面における臨界角 ζ。。が、 ファイバ光 学プレート 1の空気■コア界面における臨界角 3 C。よりも大きいので、 一部の照 明光の照明光出射面 8 4 4への入射角 ζ。は、 照明領域 8 4の空気■コア界面にお ける臨界角 。よりも小さくなる。かかる照明光は、照明光出射面 8 4 4のうち空 気と接する部分においても外部に出射することができる。そのため、照明手段が、 より効率的に、 被測定対象を照明することができる。 However, in the illumination area 84, the air 臨界 critical angle at the core interface ■. . But the critical angle 3 C in air ■ core interface of the fiber-optic plate 1. , The angle of incidence of some of the illumination light on the illumination light exit surface 84 4. Is the critical angle at the air-core interface in the illumination area 84. Smaller than. Such illumination light can also be emitted outside at a portion of the illumination light exit surface 844 that comes into contact with air. Therefore, the illumination means can more efficiently illuminate the measured object.

上記第 1ないし 3の実施形態において、 照明領域において複数のコアが配置さ れる間隔 (コアの中心軸が配置される間隔) を、 検出領域において複数のコアが 配置される間隔 (コアの中心軸が配置される間隔) よりも長くすること、 更には 照明領域のおけるコア断面積を検出領域におけるコア断面積よりも大きくするこ とが好適である。 照明領域用のマルチファイバ (M F ) 又はマルチマルチフアイ バ (MM F ) の製造に用いられる光ファイバのクラッドの厚さと、 検出領域用の マルチファイバ. (M F ) 又はマルチマルチフ了ィバ (MM F ) の製造に用い.られ る光ファイバのクラッド及び光吸収体の厚さとが同一であるとき、 照明領域にお けるコアの径を検出領域におけるコアの径よりも大きくすること、 すなわち照明 領域においてコアが配置される間隔を相対的に長くすることにより、 照明光入射 面におけるコアの面積割合が高くなり、 照明領域における照明光の入射効率が向 上する。 他方、 検出領域においてコアが配置される間隔を相対的に短くすること により、 凹凸パターン入力面及び凹凸パターン出力面における単位面積当たりの コアの本数が多くなり、 検出領域において伝送される凹凸パターンの精度が向上 する。  In the first to third embodiments, the interval at which the plurality of cores are arranged in the illumination area (the interval at which the center axis of the core is arranged) is set at the interval at which the plurality of cores are arranged at the detection area (the center axis of the core). It is preferable that the core area in the illumination area is larger than the core area in the detection area. The thickness of the cladding of the optical fiber used to manufacture the multi-fiber (MF) or multi-multi-fiber (MM F) for the illumination area and the multi-fiber for the detection area. (MF) or multi-multi-fiber (MM) When the thickness of the cladding and the light absorber of the optical fiber used in the production of F) are the same, the diameter of the core in the illumination area must be larger than the diameter of the core in the detection area, that is, the illumination area By relatively increasing the interval at which the cores are arranged in the above, the area ratio of the core on the illumination light incident surface is increased, and the incidence efficiency of the illumination light in the illumination region is improved. On the other hand, by relatively shortening the interval at which the cores are arranged in the detection area, the number of cores per unit area on the concavo-convex pattern input surface and the concavo-convex pattern output surface increases, and the concavo-convex pattern transmitted in the detection area is increased. Accuracy is improved.

上記第 1ないし 3の実施形態において、 L E Dアレーの照明方向と、 照明領域 の光伝送路の方向とがー致するように、 LEDアレーをファイバ光学プレートに 取り付けてもよい。 図 1 3は、 ファイバ光学プレート 10に LEDアレー 20が 取り付けられる態様を示す概念図である。 LEDアレー 20は、 照明方向が照明 領域 104の光伝送路の方向と一致するように、 照明光入射面 1042の下方に 配置される。 LEDアレー 20と照明光入射面 1042とは透明樹脂 30により 接合される。 検出領域 102の凹凸パターン出力面 1024に受光面 40が接合 される。 LEDアレーの照明方向と、 照明領域の光伝送路の方向とがー致するこ とにより、 照明光の照明領域 54への入射効率が向上する。 In the first to third embodiments, the illumination direction of the LED array and the illumination area The LED array may be attached to the fiber optic plate so that the direction of the light transmission path matches. FIG. 13 is a conceptual diagram showing a mode in which the LED array 20 is attached to the fiber optic plate 10. The LED array 20 is arranged below the illumination light incident surface 1042 such that the illumination direction matches the direction of the light transmission path in the illumination area 104. The LED array 20 and the illumination light incident surface 1042 are joined by the transparent resin 30. The light receiving surface 40 is bonded to the concave / convex pattern output surface 1024 of the detection region 102. When the illumination direction of the LED array matches the direction of the light transmission path in the illumination area, the efficiency with which the illumination light enters the illumination area 54 is improved.

上記第 1ないし 3の実施形態において、 照明光入射面と LEDアレーとの間に コアの屈折率、 クラッドの屈折率、 コアの中心軸に垂直な断面積、 コアが配置さ れる間隔のうち少なくとも一つが異なる別のファイバ光学プレート (中間フアイ バ光学プレート) を挟んでもよい。 図 14は、 LEDアレー 60が、 中間フアイ バ光学プレート 70を挟んで、 照明光入射面 542の下方に配置される態様を示 す概念図である。 中間ファイバ光学プレート 70は、 ファイバ光学プレート 50 と同一のスラント角が設定される。 中間ファイバ光学プレート 70を構成するコ ァ及びクラッドの屈折率を調整することにより、 照明光の照明領域 54への入射 効率を向上させることができる。 さらに、 凹凸パターン出力面 524と受光面 8 0との間にも中間ファイバ光学プレート 70を介在させてもよい。 図 1 5は、 L EDアレー 60及び受光面 80とファイバ光学プレート 50との間に中間フアイ バ光学プレート 70が介在する態様を示す概念図である。 中間ファイバ光学プレ ート 70を構成するコア及びクラッドの屈折率を調整することにより、 照明光の 照明領域 54への入射効率及び凹凸パターンの受光面 80への出力効率を向上さ せることができる。  In the first to third embodiments, at least one of the refractive index of the core, the refractive index of the clad, the cross-sectional area perpendicular to the central axis of the core, and the interval at which the core is arranged between the illumination light incident surface and the LED array Another fiber optic plate (intermediate fiber optic plate) may be sandwiched. FIG. 14 is a conceptual diagram showing a mode in which the LED array 60 is disposed below the illumination light incident surface 542 with the intermediate fiber optical plate 70 interposed therebetween. The same slant angle as the fiber optic plate 50 is set in the intermediate fiber optic plate 70. By adjusting the refractive index of the core and the cladding of the intermediate fiber optical plate 70, the efficiency of the illumination light entering the illumination area 54 can be improved. Further, an intermediate fiber optical plate 70 may be interposed between the concave / convex pattern output surface 524 and the light receiving surface 80. FIG. 15 is a conceptual diagram showing a mode in which an intermediate fiber optical plate 70 is interposed between the LED array 60 and the light receiving surface 80 and the fiber optical plate 50. By adjusting the refractive indices of the core and the clad constituting the intermediate fiber optical plate 70, it is possible to improve the efficiency with which the illumination light enters the illumination area 54 and the efficiency with which the uneven pattern is output to the light receiving surface 80. .

なお、 照明手段としては、 LEDアレー 5よりも更に薄型の埋め込み型 LED アレー 9を用いることが好適である。 図 16は、 埋め込み型 LEDアレー 9の正 面図である。 図 1 7は、 図 16に示す埋め込み型 LEDアレー 9の XVII— XVII線 に沿った断面図である。 長板形状のプリント基板 902に、 プリント基板 902 の長さ方向に沿って、 LED 904を埋め込むための埋め込み孔 906が複数形 成される。 埋め込み孔 906の底面を構成する底面板 908がプリント基板 90 2に半田で取り付けられる。 底面板 908上に LED 904が設置され、 リード 線 9 10で配線される。 LEDアレー 9を適用することにより、 より薄型の凹凸 パターン検出装置を作製することができる。 It is preferable to use an embedded LED array 9 that is thinner than the LED array 5 as the illumination means. FIG. 16 is a front view of the embedded LED array 9. Figure 17 shows the XVII-XVII line of the embedded LED array 9 shown in Figure 16. FIG. A plurality of embedding holes 906 for embedding the LEDs 904 are formed in the long board-shaped printed board 902 along the length direction of the printed board 902. A bottom plate 908 constituting the bottom surface of the embedding hole 906 is attached to the printed circuit board 902 by soldering. An LED 904 is installed on the bottom plate 908 and wired with lead wires 910. By using the LED array 9, a thinner uneven pattern detecting device can be manufactured.

産業上の利用可能性 Industrial applicability

本発明は、 例えば指紋検出器に適用可能である。  The present invention is applicable to, for example, a fingerprint detector.

Claims

請求の範囲 The scope of the claims 1 . 被測定対象の凹凸パターンを検出する凹凸パターン検出装置に適用され、 各々の軸線が双方の端面と斜めに交わり、 クラッド中に複数のコアが所定の間隔 で配置されるように、 複数の光ファイバを集成し、 成形したファイバ光学プレー トであって、  1. Applied to a concavo-convex pattern detection device that detects a concavo-convex pattern of an object to be measured, a plurality of cores are arranged at predetermined intervals so that each axis crosses both end faces at an angle and a plurality of cores are arranged at predetermined intervals in the clad. A fiber optic plate formed by assembling and forming optical fibers, 前記凹凸パターンを撮像する撮像手段が臨む検出領域と、 前記検出領域に隣接 すると共に、 前記被測定対象を照明する照明手段が臨む照明領域と、 を含んで構 成され、  A detection area facing an imaging means for imaging the concavo-convex pattern, and an illumination area adjacent to the detection area and facing illumination means for illuminating the object to be measured, 前記検出領域における前記クラッド中に、 光を吸収する光吸収体が設けられた ことを特徴とするファイバ光学プレート。  A fiber optical plate, wherein a light absorber for absorbing light is provided in the cladding in the detection region. 2 . 前記照明領域における前記クラッドの屈折率が、 前記検出領域における 前記クラッドの屈折率よりも低いことを特徴とする請求項 1記載のファイバ光学 プレート。  2. The fiber optic plate according to claim 1, wherein a refractive index of the cladding in the illumination region is lower than a refractive index of the cladding in the detection region. 3 . 前記照明領域における前記コアの屈折率が、 前記検出領域における前記 コアの屈折率よりも低いことを特徴とする請求項 1又は 2のいずれか 1項に記載 のファイバ光学プレート。  3. The fiber optic plate according to claim 1, wherein a refractive index of the core in the illumination region is lower than a refractive index of the core in the detection region. 4 . 前記照明領域において前記複数のコアが配置される間隔が、 前記検出領 域において前記複数のコアが配置される間隔よりも長いことを特徴する請求項 1 ないし 3のいずれか 1項に記載のファィバ光学プレート。  4. The interval according to any one of claims 1 to 3, wherein an interval at which the plurality of cores are arranged in the illumination area is longer than an interval at which the plurality of cores are arranged in the detection area. Fiber optical plate. 5 . 前記照明領域において前記複数のコアの中心軸が配置される間隔が、 前 記検出領域において前記複数のコアの中心軸が配置される間隔よりも長いことを 特徴する請求項 1ないし 3のいずれか 1項に記載のファイバ光学プレート。  5. The interval in which the central axes of the plurality of cores are arranged in the illumination area is longer than the interval in which the central axes of the plurality of cores are arranged in the detection area. A fiber optic plate according to any one of the preceding claims. 6 . 前記照明領域における前記複数のコアの中心軸に垂直な断面積が、 前記 検出領域における前記複数のコアの中心軸に垂直な断面積よりも大きいことを特 徴とする請求項 5記載のファイバ光学プレート。  6. The cross-sectional area perpendicular to the central axis of the plurality of cores in the illumination area is larger than the cross-sectional area perpendicular to the central axis of the plurality of cores in the detection area. Fiber optic plate. 7 . 前記照明領域が、 コアの屈折率、 クラッドの屈折率、 コアの中心軸に垂 直な断面積、 コアが配置される間隔のうち少なくとも一つが異なる複数のフアイ バ光学プレートが重ねられて構成されていることを特徴する請求項 iないし 6の いずれか 1項に記載のファイバ光学プレート。 7. The illumination area is perpendicular to the refractive index of the core, the refractive index of the clad, and the central axis of the core. The fiber optics according to any one of claims 1 to 6, wherein a plurality of fiber optic plates differing in at least one of a straight cross-sectional area and an interval at which cores are arranged are stacked. plate. 8 . 前記検出領域が、 コアの屈折率、 クラッ ドの屈折率、 コアの中心軸に垂 直な断面積、 コアが配置される間隔のうち少なくとも一つが異なる複数のフアイ バ光学プレートが重ねられて構成されていることを特徴する請求項 1ないし 7の いずれか 1項に記載のファイバ光学プレート。  8. A plurality of fiber optic plates, each having a different refractive index of the core, the refractive index of the clad, the cross-sectional area perpendicular to the central axis of the core, and the interval at which the core is disposed, are stacked. The fiber optic plate according to any one of claims 1 to 7, wherein the fiber optic plate is configured as follows. 9 . 請求項 1ないし 8のいずれか 1項に記載のファイバ光学プレートを備え、 前記撮像手段が前記検出領域の一方の表面を臨むように取り付けられ、 前記照明手段が前記照明領域の前記撮像手段が配置される側の表面を臨むよう に取り付けられる  9. A fiber optic plate according to any one of claims 1 to 8, wherein the imaging means is attached so as to face one surface of the detection area, and the illumination means is the imaging means in the illumination area. Is mounted so that it faces the surface on which the ことを特徴とする凹凸パターン検出装置。  An uneven pattern detecting device, characterized in that:
PCT/JP2003/001587 2002-02-14 2003-02-14 Fiber optical plate and irregular pattern detection device Ceased WO2003069384A1 (en)

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