会员体验
专利管家(专利管理)
工作空间(专利管理)
风险监控(情报监控)
数据分析(专利分析)
侵权分析(诉讼无效)
联系我们
交流群
官方交流:
QQ群: 891211   
微信请扫码    >>>
现在联系顾问~
热词
    • 5. 发明申请
    • COMPOUND LIGHT CONDENSING APPARATUS
    • 化合物冷凝装置
    • US20110249452A1
    • 2011-10-13
    • US12757393
    • 2010-04-09
    • Yan-Zuo ChenWen-Feng ChengTzu-Heng Chen
    • Yan-Zuo ChenWen-Feng ChengTzu-Heng Chen
    • F21V5/02
    • G02B3/08G02B19/0028G02B19/0033G02B19/0042
    • Provided is a compound light-condensing apparatus preferably including a lens body with refractive index n, and light-incident surface and light-ejected surface. The light-ejected surface has one set of Fresnel lens. When an incident light passes through the Fresnel lens structure, a focus with focal length F is formed. Two types of Fresnel lens structure are disposed on a light-ejected surface. More particularly, plural prism bodies are orderly disposed on the second type of Fresnel lens structure. The prism bodies counted from the central line is j and two adjacent prism bodies are spaced by p. The distance Tj is from a base surface to light-ejected surface. An included angle αj between ejected light and light-ejected surface is formed. By orderly changing the refractive angle of ejected light can be changed for achieving shorter focal length and better light condensation. The angle αj is formulated as: α j = 1 2  cos - 1  ( - 1 n  cos  [ tan - 1  ( 2  jp F - T j ) ] )
    • 本发明提供一种复合聚光装置,优选包括具有折射率n的透镜体和光入射面和光射出面。 光弹表面有一组菲涅尔透镜。 当入射光通过菲涅尔透镜结构时,形成具有焦距F的焦点。 两种类型的菲涅耳透镜结构设置在光射出表面上。 更具体地,多个棱镜体被有序地布置在第二类型的菲涅耳透镜结构上。 从中心线计数的棱镜体是j,两个相邻的棱镜体间隔开p。 距离Tj从基面到射出光面。 形成弹出光和光射出面之间的夹角αj。 通过有序地改变喷射光的折射角可以改变以获得更短的焦距和更好的光凝结。 角度αj表示为:αj = 1 2 cos cos(1 - 1 n cos cos(tan - 1(2 jp F - T j)])
    • 7. 发明授权
    • Non-imaging facet based optics
    • 基于非成像面的光学
    • US07697219B2
    • 2010-04-13
    • US12008053
    • 2008-01-08
    • Leo David DiDomenico
    • Leo David DiDomenico
    • G02B17/00
    • G02B5/045F24S23/10F24S23/31G02B19/0028G02B19/0033G02B19/0042G02B27/095G02B27/0977Y02E10/43
    • A high efficiency and compact optical device comprising two or more active and resonating optical facet surfaces defined by a three-dimensional representation and configured to provide a three-dimensional device. A focal region, remote from the optical surfaces and non-contiguous therewith, is defined by two or more active optical resonant surfaces, at least one of which is self-resonant. The optical surfaces in general do not have a continuous second derivative and are defined by a piecewise continuous surface function providing radially directed facets. The optical device comprises a transparent dielectric body with its optical surfaces being formed on the surfaces of said transparent dielectric body. A light transducer may be located at a focal region to provide an energy conversion. A light source having a physical extension in space, such as an LED, may be located at the focal region to provide collimation. In some embodiments the active surfaces may be chosen to transform incident radiation into a predetermined shape and having a predetermined spatial power distribution.
    • 一种高效率和紧凑的光学装置,其包括由三维表示限定并且被配置为提供三维装置的两个或更多个有源和谐振的光学小面表面。 远离光学表面并且不连续的聚焦区域由两个或更多个有源光学谐振表面限定,其中至少一个是自谐振的。 光学表面通常不具有连续的二阶导数,并且由分段连续的表面函数限定,提供径向指向的小平面。 光学器件包括透明电介质体,其光学表面形成在所述透明电介质体的表面上。 光转换器可以位于聚焦区域以提供能量转换。 在空间中具有物理延伸的光源(例如LED)可以位于焦点区域以提供准直。 在一些实施例中,可以选择有源表面以将入射辐射转换成预定形状并具有预定的空间功率分布。