| 序号 | 专利名 | 申请号 | 申请日 | 公开（公告）号 | 公开（公告）日 | 发明人 |
|---|---|---|---|---|---|---|
| 1 | 光调制器 | CN201310038784.2 | 2013-01-31 | CN103226251A | 2013-07-31 | 细川洋一; 日隈薰; 川西哲也; 菅野敦史 |
| 一种光调制器，容易实现光强度比调整。光调制器具有光调制部，光调制部具有马赫-曾德尔型光波导和调制在马赫-曾德尔型光波导中传送的光波的调制电极，如下形成整体光波导：将光调制部在同一基板上以并联状态配置多个，分支一个输入波导以连接到各光调制部的马赫-曾德尔型光波导，并且将来自马赫-曾德尔型光波导的输出合波，以一个输出波导输出，其中，向各光调制部的调制电极施加相同强度的调制信号，对至少一部分光调制部设定包括光调制部的调制电极在内的机械构造，以使由该光调制部的调制信号调制的光输出的振幅值相对于由其他光调制部通过调制信号调制的光输出的振幅值最大的最大振幅值成为1/2n。 | ||||||
| 2 | 光调制器 | CN201310038784.2 | 2013-01-31 | CN103226251B | 2017-06-13 | 细川洋一; 日隈薰; 川西哲也; 菅野敦史 |
| 一种光调制器，容易实现光强度比调整。光调制器具有光调制部，光调制部具有马赫‑曾德尔型光波导和调制在马赫‑曾德尔型光波导中传送的光波的调制电极，如下形成整体光波导：将光调制部在同一基板上以并联状态配置多个，分支一个输入波导以连接到各光调制部的马赫‑曾德尔型光波导，并且将来自马赫‑曾德尔型光波导的输出合波，以一个输出波导输出，其中，向各光调制部的调制电极施加相同强度的调制信号，对至少一部分光调制部设定包括光调制部的调制电极在内的机械构造，以使由该光调制部的调制信号调制的光输出的振幅值相对于由其他光调制部通过调制信号调制的光输出的振幅值最大的最大振幅值成为1/2n。 | ||||||
| 3 | 一种液晶显示面板 | CN201410799546.8 | 2014-12-19 | CN104503171B | 2017-06-06 | 廖作敏; 韩丙 |
| 本发明涉及一种液晶显示面板，其包括数据驱动模块，位于显示区的平行排布的数据线，位于扇出区的数据线配线，其一端连接所述数据驱动模块的输出端，其另一端连接所述显示区的数据线。其中，所述显示区中的数据线具有不同的宽度。本发明能够在液晶显示面板空间紧张无法改变扇出区数据布线的情况下，通过在显示区中设置渐变的不等线宽的数据线来代替传统的等线宽的数据线，有效地减小整个液晶显示面板上两侧数据线与中间数据线之间的阻抗差异，进而改善液晶显示面板的色偏现象。 | ||||||
| 4 | 偏振纠缠光子的三明治波导源 | CN201510753386.8 | 2011-11-10 | CN105182654A | 2015-12-23 | 罗夫·谢伦·霍恩 |
| 本公开涉及三明治波导，其包括一对基质材料，每一个基质材料中含有波导组件。多个波导组件以物理彼此接触的方式形成复合波导，从而形成三明治波导。 | ||||||
| 5 | 液晶面板及其间隙子构造 | CN201110186917.1 | 2011-07-05 | CN102243397A | 2011-11-16 | 陈雅惠; 张骢泷; 王晶 |
| 本发明公开一种液晶面板及其间隙子构造，该液晶面板包括阵列基板、彩色滤光片基板及夹设在阵列基板和彩色滤光片基板之间的多个间隙子构造，每一所述间隙子构造包含设于所述阵列基板上表面的第一间隙子及设于所述彩色滤光片基板下表面的第二间隙子。所述第二间隙子对应抵接于所述第一间隙子，当所述液晶面板受外力时，所述第一间隙子与第二间隙子抵接，从而确保所述液晶面板的显示质量。 | ||||||
| 6 | 多部件波长转换器件以及包含这些器件的激光器 | CN200880119214.3 | 2008-10-23 | CN101884147A | 2010-11-10 | J·高里尔; J·M·哈里森 |
| 根据本发明的一个实施方式，提供了一种频率转换激光源，其中，波长转换器件包括多个波导部件，这些波导部件所包括的各个输入面位于激光源的有效焦场中。各个波导部件用不同的元件促成一组不同的波长转换性质，从而定义了可归因于这些波导部件的一组不同的波长转换性质。这组不同的波长转换性质包括用于表示波导部件的相位匹配波长、波导部件的光谱宽度、波导部件的转换效率或其组合的多种性质。还揭示了其它实施方式。 | ||||||
| 7 | 叠层储存电容器结构、低温多晶硅薄膜晶体管液晶显示器 | CN200610078728.1 | 2006-05-10 | CN1979316A | 2007-06-13 | 李牧家; 黄俊伟; 吕宏哲; 郭国鸿; 李鸿斌; 赖文贵; 蔡佳怡; 张育淇; 李浩群; 张炜炽 |
| 本发明揭露一种用于低温多晶硅薄膜晶体管液晶显示器的叠层储存电容器结构，包括一基板、一第一储存电容器、及一第二储存电容器。上述第一储存电容器包括一第一导电层、一第二导电层、以及一位于该第一导电层与该第二导电层之间的第一绝缘层。此叠层储存电容器结构还包括一第三导电层，且此第三导电层包括一第一部分与一延伸的第二部分。上述第二储存电容器包括该第二导电层、该第三导电层的该延伸的第二部分、以及一位于该第二导电层与该第三导电层的该延伸的第二部分之间的第二绝缘层。 | ||||||
| 8 | 光学数模转换器 | CN200410083225.4 | 2004-09-29 | CN1652008A | 2005-08-10 | 陈阳闿; 安德瑞斯·莱文; 涂坤裕 |
| 本发明涉及通过利用连续波或脉冲激光信号来实现光学数模转换。该激光信号分成多个互相干光束，这些光束由数字数据序列的比特进行相移调制，以便转换成模拟信号。这些相移调制的光束被重新组合，以便实现想要的数模转换的光信号。 | ||||||
| 9 | 一种液晶显示面板 | CN201410799546.8 | 2014-12-19 | CN104503171A | 2015-04-08 | 廖作敏; 韩丙 |
| 本发明涉及一种液晶显示面板，其包括数据驱动模块，位于显示区的平行排布的数据线，位于扇出区的数据线配线，其一端连接所述数据驱动模块的输出端，其另一端连接所述显示区的数据线。其中，所述显示区中的数据线具有不同的宽度。本发明能够在液晶显示面板空间紧张无法改变扇出区数据布线的情况下，通过在显示区中设置渐变的不等线宽的数据线来代替传统的等线宽的数据线，有效地减小整个液晶显示面板上两侧数据线与中间数据线之间的阻抗差异，进而改善液晶显示面板的色偏现象。 | ||||||
| 10 | 偏振纠缠光子的三明治波导源 | CN201180054240.4 | 2011-11-10 | CN103201658A | 2013-07-10 | 罗夫·谢伦·霍恩 |
| 本公开涉及三明治波导，其包括一对基质材料，每一个基质材料中含有波导组件。多个波导组件以物理彼此接触的方式形成复合波导，从而形成三明治波导。 | ||||||
| 11 | 多部件波长转换器件以及包含这些器件的激光器 | CN200880119214.3 | 2008-10-23 | CN101884147B | 2012-07-18 | J·高里尔; J·M·哈里森 |
| 根据本发明的一个实施方式，提供了一种频率转换激光源，其中，波长转换器件包括多个波导部件，这些波导部件所包括的各个输入面位于激光源的有效焦场中。各个波导部件用不同的元件促成一组不同的波长转换性质，从而定义了可归因于这些波导部件的一组不同的波长转换性质。这组不同的波长转换性质包括用于表示波导部件的相位匹配波长、波导部件的光谱宽度、波导部件的转换效率或其组合的多种性质。还揭示了其它实施方式。 | ||||||
| 12 | TFT-LCD阵列基板及其制造方法 | CN201110311715.5 | 2011-10-14 | CN102360146A | 2012-02-22 | 马小龙; 陈虹瑞; 张骢泷 |
| 本发明提供了一种TFT-LCD阵列基板，包括栅极线金属层、与栅极线金属层交叠设置的数据线金属层以及包覆设置在栅极线金属层和数据线金属层周围的多个层体，栅极线金属层上设有并行且交替排列的第一栅极线和第二栅极线，数据线金属层上设有并行且交替排列的第一数据线和第二数据线；第一栅极线和第二栅极线电连接；第一数据线和第二数据线电连接。本发明还提供了一种TFT-LCD阵列基板的制造方法。实施本发明的TFT-LCD阵列基板及其制造方法，可以降低TFT–LCD有源矩阵的断线发生率，提高了产品的开口率，并且可以提高产品的良率。 | ||||||
| 13 | 파장 가변 광송신 모듈 | KR1020040081831 | 2004-10-13 | KR1020060032842A | 2006-04-18 | 박만용; 김병휘 |
| Disclosed herein is a tunable wavelength optical transmission module, the wavelength of which can be tuned over the wide wavelength region of a C band and which can be implemented at a low price and, thus, can be applied to an optical network terminal. Bragg gratings having different grating periods are arranged in parallel or series and the temperatures of Bragg grating regions are then controlled, so that the wavelength of an optical signal can be tuned over a wide wavelength range through the small variation in temperature. | ||||||
| 14 | 다층광 디스크, 다파장 광원 및 이들을 이용한 광학 시스템 | KR1020000063016 | 2000-10-25 | KR1020010070169A | 2001-07-25 | 미즈우치기미노리; 야마모토가즈히사; 고지마리에; 야마다노보루 |
| PURPOSE: An optical system using a multi-layer optical disk and a multi-wavelength light source is provided to optimize high density recording and reproducing by simultaneously emitting coherent light of multiple wavelengths varying in wavelengths. CONSTITUTION: An optical system comprises a substrate(51), plural optical waveguides(52-1,52-2) formed near the surface of the substrate, incident parts(54-1,54-2) formed at the one-side ends of the optical waveguides, and exit parts(56) formed at the other ends of the optical waveguides. The plural optical waveguides satisfy phase matching conditions varying from each other. The exit parts of the plural optical waveguides are disposed in approximately the same positions. Thereby, high density recording is realized. | ||||||
| 15 | METHOD FOR EVALUATING CHARACTERISTICS OF AN OPTICAL MODULATOR INCLUDING PLURAL MACH-ZEHNDER INTERFEROMETERS | EP10187187.9 | 2008-03-13 | EP2309323B1 | 2017-08-02 | Kawanishi, Tetsuya; Nakajima, Shinya; Shinada, Satoshi |
| 16 | ELECTRONIC PAPER AND METHOD FOR PRODUCING SAME | EP11780341.1 | 2011-04-14 | EP2570847A1 | 2013-03-20 | HIRANO, Koichi; NAKAGAWA, Masami; NAKATANI, Seiichi |
Provided is an electronic paper that permits a high-quality, large area to be easily created. Also provided is a method for producing the electronic paper. The electronic paper comprises: a first substrate upon which first electrodes are formed and a second substrate upon which second electrodes are formed, said first substrate and second substrate disposed so as to face each other; and a plurality of cell spaces constituting pixels between said first substrate and second substrate. The first substrate comprises a plurality of first sheet members, each having a first electrode formed thereon. By disposing a cover substrate on said first sheet members, each with a partition wall therebetween, a plurality of subsheet formations comprising the plurality of cell spaces partitioned by the partition walls are formed, and the first electrodes are connected in between adjacent subsheet formations. |
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| 17 | Method of evaluating the optical characteristic of a Mach-Zehnder optical modulator | EP10187187.9 | 2008-03-13 | EP2309323A2 | 2011-04-13 | Kawanishi, Tetsuya; Nakajima, Shinya; Shinada, Satoshi |
PROBLEMS To provide a method for evaluating characteristics of MZ interferometers in an optical modulator having a plurality of MZ interferometers. MEANS FOR SOLVING PROBLEMS When an optical modulator (1) includes a plurality of MZ interferometers (2,3), the output light contains a signal component at the modulation frequency and sideband components at higher orders. It is impossible to accurately evaluate the characteristic of the MZ interferometers on the basis of the component at the modulation frequency (zero-order). The present invention does not use the zero-order component normally having the highest intensity. That is, the characteristic of the MZ interferometers are evaluated by using a side band intensity of the component other than the zero-order component.
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| 18 | METHOD FOR EVALUATING CHARACTERISTIC OF OPTICAL MODULATOR HAVING MACH-ZEHNDER INTERFEROMETERS | EP08720461.6 | 2008-03-13 | EP2261628A1 | 2010-12-15 | KAWANISHI, Tetsuya; NAKAJIMA, Shinya; SHINADA, Satoshi |
PROBLEMS To provide a method for evaluating characteristics of MZ interferometers in an optical modulator having a plurality of MZ interferometers. MEANS FOR SOLVING PROBLEMS When an optical modulator includes a plurality of MZ interferometers, the 0-degree component contains a signal derived from an MZ interferometer other than the MZ interferometers for evaluating the characteristic. For this, it is impossible to accurately evaluate the characteristic of the MZ interferometers. The present invention does not use the 0-degree component normally having the highest intensity. That is, the characteristic of the MZ interferometers are evaluated by using a side band intensity of the component other than the 0-degree component. |
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| 19 | VARIABLE PATH LENGTH PASSIVE Q SWITCH | EP01928557.6 | 2001-04-16 | EP1250736B1 | 2005-01-19 | FUKUMOTO, Joseph, M. |
| A passive Q switch. The inventive Q switch (230) includes a first wedge (232) of material adapted to absorb electromagnetic energy. The first wedge (232) has a first thickness on a first end thereof and a second thickness on a second end thereof diametrically opposite the first end. The first wedge (232) has a first surface connecting the first and second ends and a second surface (236) connecting the first and second ends. The second surface (236) is slanted relative to the first surface. A second wedge of material (234) is included in the inventive passive Q switch (230). As per the first wedge (232), the second wedge (234) has a first thickness on a first end thereof and a second thickness on a second end thereof diametrically opposite the first end. The second wedge has a first surface connecting the first and second ends and a second surface (238) connecting the first and second ends. The second surface (238) is slanted relative to the first surface. The second surface (236) of the first wedge (232) is mounted in optical alignment with the second surface (238) of the second wedge (234) and in a plane parallel thereto. In the illustrative embodiment, the wedges (232, 234) are made of chromium:yttrium aluminum garnet (Cr+2:YAG) and mounted to allow the first and second wedges to translate relative to each other while maintaining a constant distant 'd' between the second surfaces thereof. The inventive Q switch allows for a variable thickness and lasing hold-off in a passive arrangement. | ||||||
| 20 | Optical multilayer disk, multiwavelength light source, and optical system using them | EP00309359.8 | 2000-10-24 | EP1096484A3 | 2004-12-22 | Mizuuchi, Kiminori; Yamamoto, Kazuhisa; Kojima, Rie; Yamada, Noboru |
When a wavelength of a first laser beam (23) with which a first recording medium (17) including a first recording layer is recorded and reproduced is indicated as λ1 (nm), a wavelength of a second laser beam (24) with which a second recording medium (18) including a second recording layer is recorded and reproduced as λ2 (nm), the relationship between the wavelength λ1 and the wavelength λ2 is set to be expressed by 10 ≦ |λ1 - λ2| ≦ 120. The first recording layer has a light absorptance ratio of at least 1.0 with respect to the wavelength λ1. The light transmittance of the first recording medium (17) with respect to the wavelength λ2 is set to be at least 30 in both the cases where the recording layer is in a crystal state and in an amorphous state. In order to record and reproduce the optical multilayer disk with the above-mentioned characteristics, a multiwavelength light source with the following configuration is used. Wavelengths of fundamental waves with different wavelengths from injection parts formed at one end of a plurality of optical waveguides, which satisfy phase matching conditions different from one another and are formed in the vicinity of the surface of a substrate, are converted simultaneously, and the first and second laser beams are emitted from emission parts formed at substantially the same position at the other end of the optical waveguides. This enables an optimum optical system for high density recording and reproduction to be obtained. |
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