WO2023047828A1 - 形状計測装置用光学系 - Google Patents
形状計測装置用光学系 Download PDFInfo
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- WO2023047828A1 WO2023047828A1 PCT/JP2022/030521 JP2022030521W WO2023047828A1 WO 2023047828 A1 WO2023047828 A1 WO 2023047828A1 JP 2022030521 W JP2022030521 W JP 2022030521W WO 2023047828 A1 WO2023047828 A1 WO 2023047828A1
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- Prior art keywords
- light
- optical system
- measured
- shape measuring
- pinhole
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- 230000003287 optical effect Effects 0.000 title claims abstract description 71
- 238000009792 diffusion process Methods 0.000 claims abstract description 23
- 238000003384 imaging method Methods 0.000 claims abstract description 18
- 239000013307 optical fiber Substances 0.000 claims description 28
- 230000002093 peripheral effect Effects 0.000 claims description 9
- 230000004907 flux Effects 0.000 claims description 6
- 230000002146 bilateral effect Effects 0.000 claims description 4
- 238000005259 measurement Methods 0.000 claims description 4
- 230000001678 irradiating effect Effects 0.000 claims description 2
- 238000010586 diagram Methods 0.000 description 5
- 230000000052 comparative effect Effects 0.000 description 4
- 230000006872 improvement Effects 0.000 description 4
- 238000012986 modification Methods 0.000 description 3
- 230000004048 modification Effects 0.000 description 3
- 239000004065 semiconductor Substances 0.000 description 3
- 239000000758 substrate Substances 0.000 description 3
- XLOMVQKBTHCTTD-UHFFFAOYSA-N Zinc monoxide Chemical compound [Zn]=O XLOMVQKBTHCTTD-UHFFFAOYSA-N 0.000 description 2
- QVQLCTNNEUAWMS-UHFFFAOYSA-N barium oxide Chemical compound [Ba]=O QVQLCTNNEUAWMS-UHFFFAOYSA-N 0.000 description 2
- 238000005516 engineering process Methods 0.000 description 2
- 239000011521 glass Substances 0.000 description 2
- OAICVXFJPJFONN-UHFFFAOYSA-N Phosphorus Chemical compound [P] OAICVXFJPJFONN-UHFFFAOYSA-N 0.000 description 1
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 description 1
- 229910052782 aluminium Inorganic materials 0.000 description 1
- 230000000903 blocking effect Effects 0.000 description 1
- 238000004364 calculation method Methods 0.000 description 1
- 229910019990 cerium-doped yttrium aluminum garnet Inorganic materials 0.000 description 1
- 238000000605 extraction Methods 0.000 description 1
- 230000002349 favourable effect Effects 0.000 description 1
- 239000000835 fiber Substances 0.000 description 1
- CPLXHLVBOLITMK-UHFFFAOYSA-N magnesium oxide Inorganic materials [Mg]=O CPLXHLVBOLITMK-UHFFFAOYSA-N 0.000 description 1
- 239000000395 magnesium oxide Substances 0.000 description 1
- AXZKOIWUVFPNLO-UHFFFAOYSA-N magnesium;oxygen(2-) Chemical compound [O-2].[Mg+2] AXZKOIWUVFPNLO-UHFFFAOYSA-N 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 239000011347 resin Substances 0.000 description 1
- 229920005989 resin Polymers 0.000 description 1
- 238000004904 shortening Methods 0.000 description 1
- 230000009466 transformation Effects 0.000 description 1
- 239000011787 zinc oxide Substances 0.000 description 1
Images
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01B—MEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
- G01B11/00—Measuring arrangements characterised by the use of optical techniques
- G01B11/24—Measuring arrangements characterised by the use of optical techniques for measuring contours or curvatures
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01B—MEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
- G01B11/00—Measuring arrangements characterised by the use of optical techniques
- G01B11/24—Measuring arrangements characterised by the use of optical techniques for measuring contours or curvatures
- G01B11/25—Measuring arrangements characterised by the use of optical techniques for measuring contours or curvatures by projecting a pattern, e.g. one or more lines, moiré fringes on the object
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01B—MEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
- G01B2210/00—Aspects not specifically covered by any group under G01B, e.g. of wheel alignment, caliper-like sensors
- G01B2210/56—Measuring geometric parameters of semiconductor structures, e.g. profile, critical dimensions or trench depth
Definitions
- the present invention is a shape measurement device used in a shape measuring device that irradiates parallel light toward an image sensor through an object to be measured and measures the two-dimensional shape of the object by using the shadow image of the object to be measured projected on the image sensor. It relates to an optical system for an apparatus.
- An optical system for a shape measuring device used in a shape measuring device that irradiates parallel light toward an image sensor through a measured object and measures the two-dimensional shape of the measured object from the shadow image of the measured object projected on the image sensor. is disclosed, for example, in US Pat.
- the optical system for a shape measuring apparatus disclosed in Patent Document 1 is arranged so as to follow the circular surface of the object to be measured and A parallel light irradiation system for irradiating parallel light so that the portion to be measured of the object to be measured is arranged in a luminous flux, and an imaging optical system for capturing a shadow image of the portion to be measured, wherein the parallel light irradiation
- the system comprises a point light source having a white LED, a collimator lens for making parallel light by making light from the point light source incident, and the light from the collimator lens being irradiated through the object to be measured, both sides or the object a telecentric lens having a side-telecentric structure, and the imaging optical system includes an image sensor on which a shadow image of the measured portion is projected by light that has passed through the telecentric lens.
- the present invention has been made in view of the circumstances described above, and an object of the present invention is to provide an optical system for a shape measuring apparatus capable of reducing luminance unevenness.
- An optical system for a shape measuring apparatus includes a parallel light irradiation system and an imaging optical system.
- the point light source includes an LED, a diffusion member that diffuses and emits the light from the LED, and a pinhole member that forms a pinhole into which the light from the diffusion member is incident.
- FIG. 1 is a schematic diagram for explaining the configuration of an optical system for a shape measuring device according to an embodiment.
- the optical system A for the shape measuring apparatus according to the embodiment irradiates parallel light toward the image sensor through the object to be measured, and the image of the object to be measured Ob projected on the image sensor determines the two-dimensional shape of the object to be measured Ob.
- An optical system used in a shape measuring apparatus for measuring for example, as shown in FIG.
- a parallel light irradiation system 1 that irradiates parallel light so that the part to be measured of the object to be measured Ob is arranged in the light flux, and an imaging that picks up a shadow image of the part to be measured. and an optical system 2 .
- the object to be measured Ob may be any member as long as it is a disk-shaped member, such as a semiconductor wafer or a hard disk substrate (aluminum substrate or glass substrate).
- the parallel light irradiation system 1 includes a point light source 11a, a collimator lens 12, and a telecentric lens 13.
- the point light source 11a includes an LED 111 (light emitting diode) 111, a diffusion member 112 (for example, an optical fiber 112a), and a pinhole member 113.
- the LED 111 is a light source that emits light.
- the diffusion member 112 is a member that diffuses and emits the light from the LED 111, and in the example shown in FIG. 1, it is an optical fiber 112a as an example thereof.
- the optical fiber 112a propagates the light from the LED 111 by repeating reflection within its core and emits the light. The light from the LED 111 is diffused by repeating this reflection.
- the optical fiber 112a is preferably in a bent shape because it can reflect more than when the optical fiber is in a straight shape. In the example shown in FIG. ).
- the diameter and the number of turns of the coil shape in the wound optical fiber 112a are suitably set according to the required diffusion of light, and in one example, the radius is about 50 mm and the number of turns is 3 or more.
- the optical fiber 112a may be made of, for example, glass or resin, and the material thereof is not particularly limited.
- the pinhole member 113 is a plate-shaped member that blocks the white light emitted from the LED 111.
- the plate-shaped member receives light from the diffusion member 112 (optical fiber 112a in this example).
- An aperture pinhole is formed.
- the diameter of the pinhole is preferably as small as possible, but if it is too small, a sufficient amount of light for shape measurement cannot be obtained. be.
- the diameter of the optical fiber 112a is preferably the same as the diameter of the pinhole, and therefore preferably within the range of 1 ⁇ m to 1 mm, more preferably within the range of 10 ⁇ m to 800 ⁇ m.
- the white light from the LED 111 is incident on the optical fiber 112a, repeatedly reflected within the core of the optical fiber 112a, propagates, is emitted from the optical fiber 112a, and enters the pinhole of the pinhole member 113. is incident.
- the collimator lens 12 is an optical system (including a single lens and a lens group) that converts the light from the point light source 11a into parallel light (parallel light flux).
- Collimator lens 12 and pinhole member 113 are arranged such that the pinhole of pinhole member 113 is positioned at the focal position of collimator lens 12 .
- the telecentric lens 13 is an optical system with a bilateral or object-side telecentric structure in which the light from the collimator lens 12 is irradiated through the object Ob to be measured.
- the telecentric lens 13 is an optical system with a telecentric structure on both sides. are aligned, and a variable stop (aperture stop) 132 is provided at this focal position.
- the telecentric lens 13 has principal rays parallel to the optical axis AX on both the object side (object to be measured Ob side) and the image side (imaging optical system 2 side). Allows only light (including light that is very nearly parallel) to pass through.
- the distance between the collimator lens 12 and the first lens 131 is set to about 200 mm, for example, and the object to be measured Ob is placed in the parallel light flux from the collimator lens 12 to the first lens 131 .
- the object to be measured Ob is preferably arranged so that the front and back surfaces thereof are parallel to the optical axis AX so that the shape of the portion to be measured, which is the outer peripheral edge portion of the object to be measured, can be preferably measured.
- the telecentric lens 13 is replaced with the above-described optical system having a telecentric structure on both sides in order to allow only parallel light (including light that is extremely parallel) to pass through the light after passing through the object to be measured Ob.
- the optical system may have an object-side telecentric structure in which the principal ray is parallel to the optical axis only on the side (object to be measured Ob side).
- a general imaging lens is used as the second lens behind the diaphragm.
- the imaging optical system 2 includes an image sensor that projects a shadow image of the portion to be measured, which is the outer peripheral edge portion of the object to be measured Ob, by the light that has passed through the telecentric lens 13 .
- the image sensor is, for example, a two-dimensional CCD image sensor, a two-dimensional CMOS image sensor, or the like.
- the parallel light irradiation system 1 configured as described above forms a better shadow image of the outer peripheral edge portion of the object to be measured Ob on the image sensor of the imaging optical system 2, even when the object to be measured Ob is not disposed. It is preferable to irradiate the parallel light so that the luminance distribution of the light irradiated to the sensor is 25% or less, and it is more preferable to irradiate the parallel light so that the luminance distribution is 20% or less. . Since the shape measuring device is optimized assuming that there is no luminance distribution, the smaller the luminance distribution, the better. However, for further improvement, it is effective to reduce the diameter of the pinhole and the fiber to make it closer to an ideal point light source. do not have. If the voltage is raised in order to obtain the required amount of light, there is a possibility that demerits such as shortening the life of the LED 111 may occur.
- a shape measuring device including the optical system A for a shape measuring device configured as described above is an image (image Data) is subjected to predetermined image processing, such as edge extraction processing for extracting edges, to extract the outer contour of the outer peripheral edge portion of the object to be measured Ob. can measure the shape of
- the optical system A for the shape measuring apparatus is provided with the point light source 11a, so that it is possible to irradiate the object to be measured with almost perfectly parallel light through the collimator lens 12, and the telecentric lens 13 allows only parallel light (including light that is extremely parallel) to pass through the light after passing through the object to be measured.
- the image sensor of the imaging optical system 2 can obtain a favorable shadow image of the outer peripheral edge portion of the object to be measured Ob with a small degree of outline blur. Therefore, even if the object to be measured Ob is, for example, a semiconductor wafer having a long depth length along the optical axis direction, the image sensor of the imaging optical system 2 has a small degree of blurring of the contour, and the outer peripheral edge of the semiconductor wafer is good. You can capture the image of the part.
- the optical system A for a shape measuring device diffuses the light from the LED 111 by the diffusion member 112, which is the optical fiber 112a in the above example, before entering the pinhole, so that uneven brightness can be reduced.
- the optical system A for a shape measuring device in which the diffusion member is an optical fiber.
- the optical fiber 112a Since the optical system A for the shape measuring apparatus in the present embodiment has a shape in which the optical fiber 112a is bent, the optical fiber 112a is more suitable than when the optical fiber has a straight shape, because the light propagates through the core with more reflections. light can be diffused evenly, and luminance unevenness can be further reduced.
- FIG. 2 is a diagram for explaining a method of calculating the luminance distribution.
- An LED 111 is used as the point light source 11a of the optical system for the shape measuring apparatus in the embodiment, an optical fiber wound three times in a coil shape with a radius of 50 mm is used as the diffusion member 112, and a pinhole member 113 has a diameter of 400 ⁇ m.
- the surface emitting LED is composed of an InGaN blue LED and a yellow YAG:Ce phosphor coated on the surface thereof.
- a collimator lens with a focal length f of 50 mm was used as the collimator lens 12, and an object-side telecentric lens with an optical magnification of 2 was used as the telecentric lens 13.
- FIG. A two-dimensional CMOS image sensor was used for the image sensor of the imaging optical system 2 .
- the object-side telecentric lens has a working distance (distance from the tip of the lens to the object to be measured): about 110 mm.
- the optical system for a shape measuring device in the comparative example has a configuration in which the diffusion member 112 (coil-shaped optical fiber 112a in the above example) is removed from the optical system for a shape measuring device in the above example.
- the luminance distribution in the optical system for the shape measuring device of the example was 11%, and the luminance distribution in the optical system for the shape measuring device of the comparative example was 26%. Therefore, the optical system for the shape measuring device of the example is improved in luminance unevenness as compared with the optical system for the shape measuring device of the comparative example.
- the luminance distribution BD is a diagonal line It was obtained from the following equation 1 using the maximum luminance Bmax and the minimum luminance Bmin in LN.
- Formula 1; BD (1-Bmin/Bmax) x 100 [%]
- the diffusion member 112 is the optical fiber 112a in the above embodiment, the diffusion member 112 may be an integrating sphere. According to this, it is possible to provide an optical system for a shape measuring apparatus in which the diffusing member is an integrating sphere.
- FIG. 3 is a schematic diagram for explaining the configuration of a modified point light source used in the optical system for the shape measuring device.
- the optical system A for a shape measuring apparatus in such a modified form includes a point light source 11b shown in FIG. 3 instead of the point light source 11a in the above configuration.
- a point light source 11 b shown in FIG. 3 includes a white LED 111 , an integrating sphere 112 b and a pinhole member 113 .
- the white LED 111 and the pinhole member 113 are the same as the white LED 111 and the pinhole member 113 described above with reference to FIG. 1, respectively, so description thereof will be omitted.
- the integrating sphere 12b is a hollow spherical member, and has an entrance opening into which the light from the white LED 111 is incident and an exit opening through which the light diffusely reflected inside the spherical member is emitted to the pinhole of the pinhole member 113.
- the white light from the white LED 111 is incident on the integrating sphere 12b via its entrance opening, diffusely reflected within the integrating sphere, and exits from the integrating sphere 112b via its exit opening. It is incident on the pinhole of the hole member 113 .
- the LED 111 may be arranged in an integrating sphere and the entrance aperture may be omitted.
- a light blocking plate is provided between the LED 111 and the exit opening so that the light from the LED 111 does not directly reach the exit opening.
- An optical system for a shape measuring apparatus is such that a portion to be measured, which is an outer peripheral edge portion of a disk-shaped object to be measured, is aligned along a circular surface of the object to be measured, and A parallel light irradiation system that irradiates parallel light so that the part to be measured is arranged in a light flux, and an imaging optical system that takes a shadow image of the part to be measured, wherein the parallel light irradiation system is a point light source and a collimator lens that converts the light from the point light source into parallel light and emits the light, and a telecentric lens that has a bilateral or object-side telecentric structure that irradiates the light from the collimator lens through the object to be measured, and the imaging
- the optical system includes an image sensor that projects a shadow image of the part to be measured by the light that has passed through the telecentric lens, and the point light source includes an LED, a diffusion member that diffuses and emits the light from the
- the parallel light irradiation system has a luminance distribution of light irradiated to the image sensor of 25% or less (more preferably 20%) when the object to be measured is not arranged. % or less).
- the light from the white LED is diffused by the diffusing member before entering the pinhole, so uneven brightness can be reduced.
- the diffusion member is an optical fiber.
- the optical fiber in another aspect, in the optical system for a shape measuring device described above, has a bent shape.
- the optical fiber has a wound shape.
- the optical fiber since the optical fiber has a bent shape, the light propagates through the core with more reflection than when the optical fiber has a straight shape, so it is more preferable. Light can be diffused, and luminance unevenness can be further reduced.
- the diffusion member is an integrating sphere.
- INDUSTRIAL APPLICABILITY it is used in a shape measuring device that irradiates parallel light toward an image sensor through an object to be measured and measures the two-dimensional shape of the object by using the shadow image of the object to be measured projected on the image sensor.
- An optical system for a shape measuring device can be provided.
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- General Physics & Mathematics (AREA)
- Engineering & Computer Science (AREA)
- Computer Vision & Pattern Recognition (AREA)
- Length Measuring Devices By Optical Means (AREA)
Abstract
Description
式1;BD=(1-Bmin/Bmax)×100[%]
Claims (4)
- 円盤状の被測定物体の外周端縁部分である被測定部に対し、前記被測定物体の円形面に沿うように、かつ、前記被測定物体の前記被測定部が光束の中に配されるように平行光を照射する平行光照射系と、
前記被測定部の影像を撮像する撮像光学系とを備え、
前記平行光照射系は、点光源と、前記点光源からの光を平行光にして射出するコリメータレンズと、前記コリメータレンズからの光が被測定物体越しに照射される、両側または物体側テレセントリック構造のテレセントリックレンズとを備え、
前記撮像光学系は、前記テレセントリックレンズを通過した光による前記被測定部の影像が投影されるイメージセンサを備え、
前記点光源は、LEDと、前記LEDからの光を拡散して射出する拡散部材と、前記拡散部材からの光が入射されるピンホールを形成したピンホール部材とを備える、
形状計測装置用光学系。 - 前記拡散部材は、光ファイバーである、
請求項1に記載の形状計測装置用光学系。 - 前記光ファイバーは、曲げられた形状である、
請求項2に記載の形状計測装置用光学系。 - 前記拡散部材は、積分球である、
請求項1に記載の形状計測装置用光学系。
Priority Applications (3)
Application Number | Priority Date | Filing Date | Title |
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KR1020247011860A KR20240054380A (ko) | 2021-09-27 | 2022-08-10 | 형상 계측 장치용 광학계 |
EP22872584.2A EP4400806A1 (en) | 2021-09-27 | 2022-08-10 | Optical system for shape measuring device |
CN202280061711.2A CN117940737A (zh) | 2021-09-27 | 2022-08-10 | 形状测量装置用光学系统 |
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JP2021-157114 | 2021-09-27 | ||
JP2021157114A JP2023047919A (ja) | 2021-09-27 | 2021-09-27 | 形状計測装置用光学系 |
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EP (1) | EP4400806A1 (ja) |
JP (1) | JP2023047919A (ja) |
KR (1) | KR20240054380A (ja) |
CN (1) | CN117940737A (ja) |
TW (1) | TWI843197B (ja) |
WO (1) | WO2023047828A1 (ja) |
Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS6217630A (ja) * | 1985-07-16 | 1987-01-26 | Nippon Kogaku Kk <Nikon> | 照明用フアイバ−束検査装置 |
JPS62294903A (ja) * | 1986-03-25 | 1987-12-22 | ドラン−ジエナ−・インダストリ−ズ・インコ−ポレ−テツド | オンライン監視のための光フアイバ像形成システム |
JP2005114499A (ja) * | 2003-10-07 | 2005-04-28 | Toppan Printing Co Ltd | ダイコートビードの検査装置及びその検査方法 |
JP4500157B2 (ja) | 2004-11-24 | 2010-07-14 | 株式会社神戸製鋼所 | 形状計測装置用光学系 |
JP2021157114A (ja) | 2020-03-27 | 2021-10-07 | 三井化学株式会社 | フォトマスク及び露光方法 |
Family Cites Families (3)
Publication number | Priority date | Publication date | Assignee | Title |
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US4772128A (en) * | 1986-03-25 | 1988-09-20 | Dolan-Jenner Industries, Inc. | Fiber optic imaging system for on-line monitoring |
JP4147169B2 (ja) * | 2003-10-17 | 2008-09-10 | 日立ビアメカニクス株式会社 | バンプ形状計測装置及びその方法 |
CN103097857B (zh) * | 2010-09-07 | 2014-12-24 | 大日本印刷株式会社 | 扫描器装置及物体的三维形状测定装置 |
-
2021
- 2021-09-27 JP JP2021157114A patent/JP2023047919A/ja active Pending
-
2022
- 2022-08-10 CN CN202280061711.2A patent/CN117940737A/zh active Pending
- 2022-08-10 KR KR1020247011860A patent/KR20240054380A/ko unknown
- 2022-08-10 EP EP22872584.2A patent/EP4400806A1/en active Pending
- 2022-08-10 WO PCT/JP2022/030521 patent/WO2023047828A1/ja active Application Filing
- 2022-09-08 TW TW111134056A patent/TWI843197B/zh active
Patent Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS6217630A (ja) * | 1985-07-16 | 1987-01-26 | Nippon Kogaku Kk <Nikon> | 照明用フアイバ−束検査装置 |
JPS62294903A (ja) * | 1986-03-25 | 1987-12-22 | ドラン−ジエナ−・インダストリ−ズ・インコ−ポレ−テツド | オンライン監視のための光フアイバ像形成システム |
JP2005114499A (ja) * | 2003-10-07 | 2005-04-28 | Toppan Printing Co Ltd | ダイコートビードの検査装置及びその検査方法 |
JP4500157B2 (ja) | 2004-11-24 | 2010-07-14 | 株式会社神戸製鋼所 | 形状計測装置用光学系 |
JP2021157114A (ja) | 2020-03-27 | 2021-10-07 | 三井化学株式会社 | フォトマスク及び露光方法 |
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JP2023047919A (ja) | 2023-04-06 |
TW202323764A (zh) | 2023-06-16 |
EP4400806A1 (en) | 2024-07-17 |
TWI843197B (zh) | 2024-05-21 |
CN117940737A (zh) | 2024-04-26 |
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