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
    • 1. 发明授权
    • Methods for making planar waveguides with removal of a sacrifical member
which surrounds the core
    • 用于制造平面波导的方法,其中移除围绕芯的牺牲部件
    • US5387269A
    • 1995-02-07
    • US115628
    • 1993-09-03
    • Casimir R. NijanderWesley P. TownsendYiu-Huen Wong
    • Casimir R. NijanderWesley P. TownsendYiu-Huen Wong
    • G02B6/136G02B6/255C03C15/00
    • G02B6/136G02B6/2552
    • An optical waveguide is made by forming successively of light transmitting material a first clad layer (13), a core layer (15) and a second clad layer (18). The core layer has a higher refractive index than that of the first and second clad layers such that the core layer (15) can transmit light along its length as an optical waveguide. A sacrificial layer (14, 17) is formed surrounding at least a first end potion of the core layer. The sacrificial layer is selectively removed as by selective etching such that the first end portion of the core layer is separated from the first and second clad layers. With the end portion so isolated, a lens (22) can be formed on it such that light may be more effectively coupled to or from the core layer. Preferably, the lens is formed by heating the structure sufficiently to form a meniscus on the free end and then cooling it before the reminder of the core layer flows or melts. The cooling hardens the meniscus such that it constitutes an optical lens.
    • 光波导通过依次形成第一覆层(13),芯层(15)和第二覆层(18)而形成透光材料。 芯层具有比第一和第二包层更高的折射率,使得芯层(15)可以沿着其长度透射光作为光波导。 形成围绕芯层的至少第一端部的牺牲层(14,17)。 通过选择性蚀刻选择性地去除牺牲层,使得芯层的第一端部与第一和第二覆盖层分离。 在端部如此隔离的情况下,可以在其上形成透镜(22),使得光可以更有效地耦合到芯层或从芯层耦合。 优选地,通过将​​结构充分加热以在自由端上形成弯液面并然后在芯层的提醒流动或熔化之前将其冷却来形成透镜。 冷却使弯液面硬化从而构成光学透镜。
    • 3. 发明授权
    • Method for making microstructures
    • 制造微结构的方法
    • US5370768A
    • 1994-12-06
    • US135644
    • 1993-10-14
    • Keith O. MersereauCasimir R. NijanderWesley P. Townsend
    • Keith O. MersereauCasimir R. NijanderWesley P. Townsend
    • G02B3/00B44C1/22C03C15/00C03C25/06H01L21/306
    • G02B3/0018G02B3/0056
    • Prior to the production of microlenses (29) by the reactive ion etch technique, a pattern of notches (25) is formed in a second surface of a substrate (11) opposite a first surface on which the microlenses (29) are to be formed. Reactive ion etching of the first surface to produce the microlenses is sufficiently deep to reach the pattern of notches, thereby to separate the substrate. The array of notches may define, for example, an array of first areas (26) on the second surface, each area being surrounded by a notch. Photoresist elements (28) are then each located on an area of the first surface corresponding to a first area of the second surface, so that the separation separates the substrate into a plurality of segments (26) each containing only one of the microlenses (29). The notches can be made such that each of the segments (26) is cylindrical so that each of the microlenses formed from the substrate has a circular outer periphery.
    • 在通过反应离子蚀刻技术生产微透镜(29)之前,在与要在其上形成微透镜(29)的第一表面相对的衬底(11)的第二表面中形成凹口(25)的图案 。 第一表面的反应离子蚀刻以产生微透镜足够深以达到凹口的图案,从而分离衬底。 凹口阵列可以例如限定第二表面上的第一区域(26)的阵列,每个区域被凹口包围。 光阻元件(28)然后各自位于与第二表面的第一区域对应的第一表面的区域上,使得该分离将基板分离成多个段(26),每个段仅包含一个微透镜(29 )。 可以制成切口,使得每个片段(26)是圆柱形的,使得由基底形成的每个微透镜具有圆形的外周边。
    • 5. 发明授权
    • Methods for making microstructures
    • 制作微结构的方法
    • US5439782A
    • 1995-08-08
    • US165203
    • 1993-12-13
    • William H. HaemmerleWilliam M. MacDonaldCasimir R. NijanderJoseph ShmulovichWesley P. TownsendYiu-Huen Wong
    • William H. HaemmerleWilliam M. MacDonaldCasimir R. NijanderJoseph ShmulovichWesley P. TownsendYiu-Huen Wong
    • C23F4/00G02B6/122G02B6/13G02B6/30G02B6/12
    • G02B6/1228G02B6/1221G02B6/305
    • Tapered optical waveguides (33') can be easily made by using photolithographic masking and etching to define on a substrate (21) a first polymer structure (22) having a substantially uniform thickness and a tapered width. The first polymer structure is heated sufficiently to form a meniscus along its entire length. The fluidity causes the material to redistribute itself such that, rather than being of uniform thickness, it has a thickness that varies with its width; consequently, the thickness as well as the width of the first polymer structure becomes tapered. The first polymer is cooled and hardened to form a second polymer structure (22') that has a tapered width and a tapered thickness as is desirable for a tapered optical waveguide. The second polymer structure itself can be used as a tapered optical waveguide, or it can be used to control the reactive ion etching of the underlying substrate. In the latter case, the configuration of the tapered second polymer structure is replicated in a glass substrate, for example, which then may be used as a glass tapered optical waveguide (33').
    • 锥形光波导(33')可以通过使用光刻掩模和蚀刻来在衬底(21)上限定具有基本上均匀的厚度和锥形宽度的第一聚合物结构(22)来容易地制成。 第一聚合物结构被充分加热以在整个长度上形成弯液面。 流动性导致材料重新分布自身,使得不是具有均匀的厚度,而是具有随其宽度而变化的厚度; 因此,第一聚合物结构的厚度以及宽度变得逐渐变细。 将第一聚合物冷却并硬化以形成第二聚合物结构(22'),其具有如锥形光波导所需的锥形宽度和锥形厚度。 第二聚合物结构本身可以用作锥形光波导,或者可以用于控制底层基板的反应离子蚀刻。 在后一种情况下,锥形第二聚合物结构的构造被复制在例如可用作玻璃锥形光波导(33')的玻璃基板中。