序号 专利名 申请号 申请日 公开(公告)号 公开(公告)日 发明人
181 Lens for illumination device EP14000020.9 2014-01-03 EP2891915A1 2015-07-08 Yeh, Chien Hung

A lens for an illumination device includes a lens 1 having a first surface 11 and a second surface 12 connected to each other along an annular curved line 14 which is composed of two symmetric curved lines 15. The two symmetric curved lines 15 are connected to each other at a first point 151 and a second point 153. Each of the two curved lines 15 has a middle point 152. The first surface 11 is a multiple-focus surface and located on the outer side of the lens 1. The patterns and paths of the light beams can be controlled by the first surface 11 of the lens 1.

182 Refractive optical element having a convex helical surface for athermalizing an infrared imaging system EP13460040.2 2013-06-27 EP2778732A1 2014-09-17 Sypek, Maciej; Blocki, Narcyz; Kolodziejczyk, Andrzej; Jaroszewicz, Zbigniew

Refractive optical element for athermalizing an infrared imaging system, said element being detachably mounted to the latter and having a circular base and a convex surface with an helical profile, the radial jog of which ascending helically from the lower edge (1) to the upper edge (2) of the jog.

183 LINSE MIT EINEM ERWEITERTEN FOKUSBEREICH EP12723377.3 2012-05-16 EP2710426A1 2014-03-26 DOBSCHAL, Hans-Jürgen
The invention relates to a lens that has an extended focal range, said lens consisting of a solid material. The optical surfaces of the lens are transparent, and the lens has a refractive index distribution. According to the invention, the refractive index distribution F G of the lens (1) with respect to a plane that is perpendicular to the optical axis (10) changes between a refractive index base value F L that is not equal to zero and a maximum value F Smax as a function of the radial height r and the azimuth angle phi of the aperture. Thus, the refractive index distribution results from FG(r,phi) = FL + FS (r,phi), with the spiral-shaped refractive index portion FS(r,phi) = FS max(r) * w(phi), wherein F Smax(r) is nonlinearly dependent on the radius and w(phi) is a factor for the refractive index portion with a spiral curve.
184 IMAGING OPTICS DESIGNED BY THE SIMULTANEOUS MULTIPLE SURFACE METHOD EP09805286 2009-08-07 EP2316046A4 2014-03-26 MINANO JUAN CARLOS; BENITEZ PABLO; MUNOZ FERNANDO
185 LIGHT EMITTING DEVICE AND ILLUMINATING DEVICE PROVIDED WITH THE SAME EP08827067 2008-08-08 EP2175193A4 2012-10-17 KOKUBO FUMIO
A light-emitting device (10) includes: a light-emitting element (1); and a light flux controlling member (2) for controlling light emitted from the light-emitting element (1), the light flux controlling member (2) has (i) a light-incoming surface (2a) which the light emitted from the light-emitting element (1) enters and (ii) a light-outgoing surface (2b), and the following equation (1) is satisfied where r is a length, from a light axis Z of the light-emitting device (10), of a plane that is provided at a certain distance from the light flux controlling member (2) in a direction parallel to the light axis Z so as to be perpendicular to the light axis Z, Æ 1 is an angle between the light emitted from the light-emitting element (1) and the light axis, P(Æ 1 ) is a light distribution property of the light-emitting element (1). This provides a light-emitting device that scatters light without generating uneven brightness on a liquid crystal display panel, reduces a reflectance caused by the Fresnel's reflection, and has an improved scattering ability.
186 METHOD OF MEASURING A SHAPE OF AN OPTICAL SURFACE AND INTERFEROMETRIC MEASURING DEVICE EP09778606.5 2009-09-18 EP2478328A1 2012-07-25 FREIMANN, Rolf; DÖRBAND, Bernd; SCHULTE, Stefan; HOF, Albrecht; RIEPENHAUSEN, Frank; MANGER, Matthias; NEUGEBAUER, Dietmar; ISSLER, Helmut; BICH, Armin
A method of measuring a shape of an optical surface (14) of a test object (12) is provided. The method comprises the steps of: providing an interferometric measuring device (16) generating a measurement wave (18), arranging the interferometric measuring device (16) and the test object (12) consecutively at different measurement positions relative to each other, such that different regions (20) of the optical surface (14) are illuminated by the measurement wave (18), measuring the positional coordinates of the measuring device (16) at the different measurement positions in relation to the test object (12), obtaining surface region measurements by interferometrically measuring the wavefront of the measurement wave (18) after interaction with the respective region (20) of the optica! surface (14) using the measuring device (16) in each of the measurement positions, and determining the actual shape of the optical surface (14) by computationally combining the sub-surface measurements based on the measured positional coordinates of the interferometric measuring device (16) at each of the measurement positions.
187 Luminaire and method of operation EP09161287.9 2009-05-27 EP2128660B1 2012-04-18 Bailey, Edward
188 DISPLAY DEVICE AND ELECTRONIC DEVICE EP09769871 2009-06-18 EP2306437A4 2011-12-21 WATANABE HISASHI; SHIBATA SATOSHI
189 Oblique projection optical system and projection type display apparatus using the same EP09252803.3 2009-12-16 EP2209024A3 2010-09-01 Hirata, Koji; Yatsu, Masahiko; Ogura, Naoyuki

A projection type display apparatus including an oblique projection optical system having a plurality of lenses is disclosed. A lens nearest to a projection screen has a vertical effective image area through which a light flux (3) passes. The lens is arranged at a position not including an optical axis (11) shared by the largest number of lenses among the plurality of lenses. A flat mirror (14) for returning the optical path is arranged between the particular lens and the projection screen at a predetermined angle to the optical axis (11). An enlarged image obtained by the light flux (3) returned by the flat mirror (14) is formed toward a display screen.

190 Collimation lens system for led EP09252825.6 2009-12-18 EP2202455A1 2010-06-30 Chu, Man Yin Arthur Newton; Zhang, Jingdong; Jiang, Jingbo; To, Suet

A collimation lens system (100) for converging the light from an LED (30) into a light beam (L), comprises:

a central lens (10) aligned along an optical axis (X) with the LED (30) for converging inner light from the LED (30), the central lens (10) comprising an aspheric collimation plano convex lens (10) having a planar entrance surface (11) and an aspheric exit surface (12); and

a peripheral lens (20) surrounding the central lens (10) for converging outer light from the LED (30), the peripheral lens (20) comprising a total internal reflection collimation lens having an entrance surface (21) and an exit surface (22) and including a high order aspheric total internal reflection surface (23) for reflecting said outer light by way of total internal reflection.

The central lens (10) and the peripheral lens (20) share a common focal point at which the LED (30) may be positioned.

191 Luminaire and method of operation EP09161287.9 2009-05-27 EP2128660A1 2009-12-02 Bailey, Edward

A luminaire and a method of operating a luminaire is provided. The luminaire includes a light source emitting a plurality of light rays. A collimation device is arranged to receive a portion of light from the light source and transmits the portion of light through an exit aperture towards an illuminated area. The exit aperture includes a planar portion and at least one lenslet formed thereon. The lenslet is arranged having a first profile and a second profile, where the portion of light is refracted on a plurality of angles to form a twisted profile by the lenslet.

192 Focusing lens for LED EP07104358.2 2007-03-16 EP1962013A1 2008-08-27 KIM, Jin-Ho; HWANG, Shung-Hoon; LEE, Hee-Joong

A focusing lens (100) for an LED (2), which concentrates light emitted from the LED (2) so as to have directionality parallel to an optic axis (4), comprises: a transparent body (110); a first lens part (200) formed in the body; and a second lens part (300) covering the first lens part (200), and wherein the first lens part (200) comprises: parallel first and second convex aspheric lens surfaces (210,220), and wherein the second lens part (300) comprises: a plane of incidence (310) formed to protrude from an outer circumference of the first aspheric lens surface (210), the plane of incidence (310) into which the LED (2) is inserted and which is configured to allow the light emitted from the LED (2) to be incident and refracted; a plane of reflection (320) formed to have a convex curved surface which extend and slopes to be progressive wider from the plane of incidence (310) towards the second aspheric lens surface (220), the plane of reflection (320) which is configured to allow the light emitted from the LED (2) to be totally reflected; and a plane of emission (330) formed to have a concave curved surface which extends and slopes from the plane of reflection (320) towards the second aspheric lens surface (220), the plane of emission (330) which is configured to allow the light emitted from the LED (2) to be refracted and emitted as light being parallel to the optic axis (4). The focusing lens minimizes loss of the light emitted from the LED (2) and maximally reduces an angle of the emitted light, to effectively illuminate a local region at a long distance.

193 An optical device and an optical lens EP06256198.0 2006-12-05 EP1795863A2 2007-06-13 Munroe, Jay; Li, Haizhang; Liu, Yaping

A non-cylindrically surfaced lens converts a collimated light beam into a light plane that increases a light intensity toward distal portions of the light plane's arc so as to substantially uniformly project a reference light line onto a reference surface onto which the light plane is projected. The non-cylindrically surfaced lens has first and second surfaces that remain constant over at least a portion of the z direction length of the lens. The second surface defines a multiple-radius curve in an x,y plane. The lens may be incorporated into a self-leveled optical device that projects a reference light line onto a reference surface at a predetermined angle relative to horizontal.

194 OPTICAL DEVICE PROVIDED WITH OPTICAL ELEMENT FORMED OF MEDIUM EXHIBITING NEGATIVE REFRACTION EP05782219.9 2005-09-06 EP1788418A1 2007-05-23 NISHIOKA, Kimihiko Intellectual Property Supp.Dept.

A lens is disclosed. The lens includes an optical element made of a material exhibiting a positive refractive index, and a medium exhibiting negative refraction formed on the optical element serving as a substrate.

195 BICONVEX SOLID IMMERSION LENS EP02806615.7 2002-12-11 EP1466194B1 2007-04-04 Nader, Pakdaman; Vickers, James S.
A bi-convex solid immersion lens is disclosed. Unlike conventional plano-convex solid immersion lenses having a flat bottom surface, the disclosed lens has a convex bottom surface. The radius of curvature of the bottom surface is smaller than that of the object to be inspected. This construction allows for a more accurate determination of the location of the inspected feature, and enhances coupling of light between the immersion lens and the inspected object. The disclosed lens is particularly useful for use in microscope for inspection of semiconductor devices and, especially flip-chip (or chip scale) packaged devices. The immersion lens can also be incorporated in a read or read/write head of optical memory media.
196 ASPHERICAL MICROLENS ARRAYS AND FABRICATION METHOD THEREOF AND APPLICATIONS USING THE SAME EP04808554.2 2004-12-23 EP1704425A2 2006-09-27 YEE, Young-Joo; LEE, Gun-Woo; PARK, Ki-Won, Gwanakdongsung Apt. 114-704; SEONG, Dong-Mug
An aspherical microlens arrays (100) comprise a base (120), and a plurality of aspherical microlens (110) arranged on the base (120) and having different curvature radiuse and conic coefficient respectively, along two orthogonal axes on the base (120) perpendicular to an optical axis, by which a degree of refraction, namely, a numerical aperture can be easily adjusted depending on each axial direction, a spherical aberration can be reduced, and concentration efficiency can be improved. In addition, in case of applying the aspherical microlens arrays (100) to a projection screen, an image sensor, or the like, it is advantageous to improve sensitivity and resolution thereof.
197 Selectable beam lens for underwater light EP05110078.2 2005-10-27 EP1653255A2 2006-05-03 Potucek, Kevin; Dunn, Dennis

A lens for a wet environment lighting device that has a fixture with an interior that has an opening, and at least one light source located within the fixture interior. Light from the light source proceeds out through the opening. The lens is for location in front of the fixture and the light source located therein and the lens encloses the opening from the wet environment. The lens has a first light-directing area for directing light in a first beam pattern. The lens also has a second light-directing area, distinct from the first light-directing area, for directing light in a second beam pattern, distinct from the first beam pattern. The lens is positioned relative to fixture and light source therein to select from the distinct beam patterns based on the alignment of the light-directing areas relative to the light source resulting from a positioning of the lens.

198 OPTICAL ELEMENT EP04745801.3 2004-06-11 EP1635194A1 2006-03-15 MATAKI, Hiroshi, c/o KRI, Inc.; FUKUI, Toshimi, c/o KRI, Inc.

The present invention provides an athermalized optical element that does not require auxiliary material to compensate for the rate of change of the refractive index with temperature, which can be widely applied to both transparent materials of inorganic material and organic material, and is formed without decrease of transparency and dimension distortion.

The optical element of the present invention is an optical element for controlling light propagation including: transparent material; and inorganic fine particles dispersed in the transparent material, wherein the transparent material and the inorganic fine particles meet at least one of following a) and b):

  • a) a rate of change of a refractive index of the transparent material with temperature and a rate of change of a refractive index of the inorganic fine particles with temperature are opposite in sign;
  • b) a thermal expansion coefficient of the transparent material and a thermal expansion coefficient of the inorganic fine particles are opposite in sign.

199 COMPACT FOLDED-OPTICS ILLUMINATION LENS EP03774742.5 2003-10-10 EP1556715A2 2005-07-27 BENITEZ, Pablo; MINANO, Juan, C.; MUNOZ, Fernando
A method for manufacturing an apparatus and the apparatus being configured to convert a first distribution of an input radiation to a second distribution of output radiation. The method consists of the steps of generating a two-dimensional representation of at least three active optical surfaces of an optical device including calculating a segment of a first surface based on edge ray sets as a first generalized Cartesian oval, calculating a segment of an entry surface based on the edge ray set as a second generalized Cartesian oval, calculating a segment of a second surface based on the edge ray set as a third generalized Cartesian oval, and successively repeating the steps of calculating the segment of the first surface and calculating the segment of the second surface in a direction towards a source, and rotationally sweeping the two-dimensional representation about a central axis providing a three-dimensional representation of the optical device.
200 Resin-made convex cone mirror for projecting a reference laser beam EP02256493.4 2002-09-19 EP1296163B1 2004-12-01 Terauchi, Isshu; Teraji, Norihisa
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