| 序号 | 专利名 | 申请号 | 申请日 | 公开（公告）号 | 公开（公告）日 | 发明人 |
|---|---|---|---|---|---|---|
| 81 | CAMERA MODULE | EP16864543.0 | 2016-11-09 | EP3376284A1 | 2018-09-19 | YANG, Jun Suk; PARK, Ok Hyeon; LEE, Min Woo; HAN, Sang Yeal |
A camera module comprises: a housing comprising a housing body and a cable fixing body which extends from the housing body and has an engaging part formed therein; a camera main body coupled with a cable which passes through the cable fixing body; a cable fixing member, a part of which is press-fitted into the outer circumferential surface of the cable and the other part of which is caught in the engaging part; and a waterproof member inserted and fixed in the cable fixing body while being coupled with the cable. |
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| 82 | WAVELENGTH SEPARATING BEAMSPLITTER | EP09770967 | 2009-06-24 | EP2307917A4 | 2016-05-25 | TOWNDROW CLIVE; CALDWELL BRIAN |
| A prism system is disclosed for splitting a broadband incoming light beam. In one embodiment, the broadband beam enters the prism system and is shifted laterally through a parallelogram shaped prism. The beam then encounters a first dichroic coating treated surface. The light that is reflected off of the surface strikes the internal wall of the prism to undergo total internal reflection within the prism. The beam exits the prism parallel to the original incoming broadband beam. The beam that passes through the dichroic surface reaches a second dichroic coating treated surface where a specified waveband of light is reflected while the remaining wavelengths pass through. The beam reflected by the second dichroic surface undergoes a total internal reflection and exits parallel to the incoming broadband beam. The light beam which passes through the second dichroic surface exits the prism parallel to the original incoming broadband beam. | ||||||
| 83 | IMAGING OPTICAL SYSTEM AND PROJECTION EXPOSURE APPARATUS THEREWITH | EP12171864.7 | 2008-10-02 | EP2533104B1 | 2016-05-11 | MANN, Hans-Jürgen |
| 84 | IMAGING OPTICAL SYSTEM AND PROJECTION EXPOSURE INSTALLATION FOR MICRO-LITHOGRAPHY WITH AN IMAGING OPTICAL SYSTEM OF THIS TYPE | EP08802769.3 | 2008-10-02 | EP2203787B1 | 2014-05-14 | MANN, Hans-Jürgen |
| 85 | APPARATUS AND METHOD FOR VIEWING AND INSPECTING A CIRCUMFERENTIAL SURFACE AREA OF AN OBJECT | EP98956274.9 | 1998-10-28 | EP1027590B1 | 2009-06-03 | MEHROTRA, Yogesh; PIKE, John, Nazarian; KAPLAN, Herbert |
| An apparatus (10) and method are provided for viewing of a surface area of a three-dimensional object (D) and for inspecting the surface area for flaws or imperfection. A receiving lens (12) defines an optical axis (14) extending through the object for generating a direct image of a front surface section of the object. A first mirror (16) is spaced a first predetermined distance (L1) from an origin (0) on another side of the object relative to the receiving lens (12) for generating a first mirror image of a first rear surface of the object. A second mirror (18) is spaced a second predetermined distance (L2) from the origin (0) on another side of the optical axis (14) relative to the first mirror, for generating a second mirror image of a second rear surface section of the object. The first and second predetermined distances (L1, L2) and the angles of incidence of the mirrors are each selected to simultaneously generate at least three spatially distinct, non-vignetting images forming a 360 DEG view of the surface area. | ||||||
| 86 | OPTICAL SYSTEM, METHOD OF ALTERING RETARDANCES THEREIN AND PHOTOLITHOGRAPHY TOOL | EP03722501.8 | 2003-04-17 | EP1614007A1 | 2006-01-11 | KAMENOV, Vladimir; GRUNER, Toralf |
| An optical system, for example a lens for a photolithography tool, includes a group of optical elements (L1, L2) that each comprise a birefringent cubic crystal such as CaF2. The crystal lattices of the crystals have different orientations, e.g. for reducing the overall retardance of the group by mutual compensation. The [110] crystal axis of at least one optical element (L1, L2) is tilted with respect to an optical axis (34) of the system (10) by a predefined tilting angle (θ1, θ2) having an absolute value between 1° and 20°. This reduces the magnitude, but not significantly change the orientation of intrinsic birefringence. By selecting an appropriate tilting angle it is possible to achieve a better performance of the optical system. For example, the overall retardance of the optical system may be reduced, or the angular retardance distribution may be symmetrized. | ||||||
| 87 | A focusing-device for the radiation from a light source | EP04022998.1 | 2004-09-28 | EP1521119A3 | 2006-01-04 | Antoni, Martin; Melzer, Frank; Seifert, Andreas; Singer, Wolfgang |
A focusing-device for the radiation from a light source (2) is provided with a collector mirror (1, 1') which is arranged in a mount (24) and collects the light, in virtual or real terms, from the light source (2) at the second focus (200). The collector mirror (1, 1') is displaceably connected to the mount (24) via a bearing in such a way that the collector mirror can be displaced at least perpendicular to the optical axis (35). |
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| 88 | APPARATUS AND METHOD FOR VIEWING AND INSPECTING A CIRCUMFERENTIAL SURFACE AREA OF AN OBJECT | EP98956274 | 1998-10-28 | EP1027590A4 | 2001-12-05 | MEHROTRA YOGESH; PIKE JOHN NAZARIAN; KAPLAN HERBERT |
| An apparatus (10) and method are provided for viewing of a surface area of a three-dimensional object (D) and for inspecting the surface area for flaws or imperfection. A receiving lens (12) defines an optical axis (14) extending through the object for generating a direct image of a front surface section of the object. A first mirror (16) is spaced a first predetermined distance (L1) from an origin (0) on another side of the object relative to the receiving lens (12) for generating a first mirror image of a first rear surface of the object. A second mirror (18) is spaced a second predetermined distance (L2) from the origin (0) on another side of the optical axis (14) relative to the first mirror, for generating a second mirror image of a second rear surface section of the object. The first and second predetermined distances (L1, L2) and the angles of incidence of the mirrors are each selected to simultaneously generate at least three spatially distinct, non-vignetting images forming a 360 DEG view of the surface area. | ||||||
| 89 | Sun-observation device | EP99200248.5 | 1999-01-29 | EP0927902A3 | 1999-07-28 | Lock, Herbert Martin |
A device for direct viewing of the sun comprises a body member defining a housing including an objective aperture and a viewing aperture, the housing containing light-absorbing reflection means arrange to define a light pathway between said objective and viewing apertures, whereby total light transmittance is attenuated to an extent such as to enable the sun to be observed with safety. |
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| 90 | Binocular reflecting telescope | EP93119803.0 | 1993-12-08 | EP0601565B1 | 1998-03-25 | Masunaga, Shuichi; Masunaga, Sumie |
| 91 | IMAGE ROTATION DEVICE | EP92921724.0 | 1992-10-06 | EP0694177A1 | 1996-01-31 | SUDARSHAN, E., C., George; HULET, Randall, G. |
| An optical rotation device (10) with infinite depth of field for transmitting optical images along an optical axis and selectively rotating the image (26) about the optical axis, while preserving all of the three dimensional characteristics of the image. The optical rotation device consists of two optical elements (12, 14) optically coupled in series, each of which produces an inversion of the image about an axis orthogonal to the optical axis. Rotation of the image by any angle in the plane normal to the optical axis is achieved by rotating the two optical elements relative to one another about the optical axis. | ||||||
| 92 | Thermal imager systems | EP92301066.4 | 1992-02-07 | EP0499421B1 | 1995-11-08 | Smith, Brian Frederick; Cuthbertson, Glenn McPherson |
| 93 | Strahlungsführungsoptik für Laserstrahlung | EP87114094.3 | 1987-09-26 | EP0283555B1 | 1993-08-11 | Gorisch, Wolfram, Dr. |
| 94 | Optical image rotators | EP88307537.6 | 1988-08-15 | EP0307094B1 | 1993-03-24 | Keens, Andrew Peter |
| 95 | METHODS OF AND APPARATUS FOR MANIPULATING ELECTROMAGNETIC PHENOMENON | EP90913081 | 1990-08-21 | EP0487612A4 | 1993-01-20 | AMOS, CARL, R. |
| Methods of and apparatus for manipulating beamed electromagnetic phenomenon comprise a generator (20) of aligned conical or pyramidal elements (21a-21f) each having conical or pyramidal inner and outer surfaces (24a-24f and 23a-23f). When the beamed electromagnetic phenomenon includes a zero-order component the elements (21a-21f) minimize or eliminate the zero-order component allowing for devices such as on-axis holographic displays, demodulators and optical processors for computers. | ||||||
| 96 | Thermal imager systems | EP92301066.4 | 1992-02-07 | EP0499421A1 | 1992-08-19 | Smith, Brian Frederick; Cuthbertson, Glenn McPherson |
A thermal imager system comprises a scanning system 1 for scanning a required scene 2 and an anamorphic optical system 3 for focusing the scanned scene onto a Sprite detector 4, the optical anamorphic system comprises a pair of optical prisms 17, 19 disposed between a collimating element 15 and a focusing element 21, one or both of the prisms 17, 19 being pivotally mounted whereby the anamorphic ratio and hence the focal length of said optical system 3 may be changed. |
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| 97 | LENSES FOR PHOTOGRAPHIC PRINTERS | EP87903652.3 | 1987-05-21 | EP0302081B1 | 1992-08-05 | ESTELLE, Lee, Roy |
| A lens device for a photographic printer to enable it to print same size prints from full-frame and half-frame images intermixed in an elongate strip of spliced film strips. If the lens device is one of two and is dedicated to printing half-frame images, the lens device rotates the image through 90° without affecting the inversion and reversion needed in a printer lens. The device includes a pechan prism in each of the air spaces between the lens elements and the object and image planes, respectively. There is a relative angular displacement of 45° between the prisms. The device enlarges the image more than the other lens, which is dedicated to full-frame images, so that images printed by both lenses have the same size. If the lens device is the only lens in the printer, then it is a zoom lens, so that images from both full and half-frame may be the same size, and the relative angular displacement between the prisms is variable so that both full and half-frame may be printed on the paper web with the same orientation on the web. | ||||||
| 98 | A METHOD OF ARRANGING THE RAY PATH IN AN OPTICAL INSTRUMENT | EP90913183.0 | 1990-08-21 | EP0489095A1 | 1992-06-10 | STRÖMBERG, Rolf |
| L'invention concerne une méthode pour arranger la trajectoire lumineuse dans un instrument monoculaire, binoculaire ou semblable (7) de manière à réaliser un instrument le plus compact et le plus ergonomique possible, tout en maintenant les meilleures données optiques possibles, et en utilisant des miroirs internes (1-4) aux plus petites dimensions. On situe la trajectoire près d'un plan, au moins deux (2, 3) des miroirs pour redresser l'image étant placés de chaque côté dudit plan. La lumière provenant de l'objectif (6) est incidente sur chaque miroir (2, 3) l'un après l'autre, l'inclinaison de l'image étant éliminée en inclinant la ligne d'intersection desdits deux miroirs (2, 3) par rapport au plan. | ||||||
| 99 | METHODS OF AND APPARATUS FOR MANIPULATING ELECTROMAGNETIC PHENOMENON | EP90913081.0 | 1990-08-21 | EP0487612A1 | 1992-06-03 | AMOS, Carl, R. |
| Procédés et appareil de manipulation de phénomène électromagnétique sous forme de faisceau, comprenant un générateur (20) d'éléments (21a à 21f) coniques ou pyramidaux alignés, ayant chacun des surfaces (24a à 24f et 23a à 23f) intérieures et extérieures coniques ou pyramidales. Lorsque le phénomène électromagnétique sous forme de faisceau comprend un composant d'ordre zéro, les éléments (21a à 21f) réduisent au minimum ou éliminent la composante d'ordre zéro ce qui permet à des ordinateurs d'utiliser des dispositifs tels que des affichages holographiques, des démodulateurs et des processeurs optiques axiaux. | ||||||
| 100 | An apparatus for rotating a light image and an optical system for focusing light beams on a recording medium | EP89100155.4 | 1989-01-05 | EP0323845A3 | 1989-11-23 | Yamanaka, Yutaka |
An apparatus for rotating a light image comprises an optical medium such as a Dove prism, an assembly of three mirrors, a triangle prism etc., and a unit (24) for rotating the optical medium. The optical medium is provided with n reflection planes in number each having a normal included in a predetermined plane including a reference light axis, where n is an odd number (n = 1, 3, 5 ...). When an incident light beam parallel to the reference light axis is supplied to the optical medium, an output light beam having a predetermined rotating angle relative to the incident light beam is obtained by rotating the optical medium around a line parallel to the reference light axis. An optical system for focusing a light image further comprises a light source (21) for radiating a plurality of light beams, and a focusing lens (25) for focusing the light beams on a recording medium (27) such as an optical disk, a photosensitive drum etc. The optical medium is positioned between the light (21) and the focusing lens (25), so that a line connecting beam spots formed on the recording medium (27) by focusing the lgiht beams is rotated by rotating the optical medium. |
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