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
    • 11. 发明申请
    • Photonic crystal having heterostructure and optical device using the photonic crystal
    • 具有异质结构的光子晶体和使用光子晶体的光学器件
    • US20090175572A1
    • 2009-07-09
    • US10584942
    • 2005-03-24
    • Susumu NodaTakashi AsanoSeiichi Takayama
    • Susumu NodaTakashi AsanoSeiichi Takayama
    • G02B6/12
    • B82Y20/00G02B6/12004G02B6/1225
    • The present invention has been made for providing a photonic crystal capable of multiplexing or demultiplexing light within a wavelength band having a certain width. It includes a slab-shaped body 21 provided with plural forbidden band zones 211 and 212, and holes 221 and 222 having different sizes are arranged in the forbidden band zones with different cycles, respectively. Also formed are a trunk waveguide 24 extending along the direction inclined by +30 degrees from a perpendicular of the boundary 23 between the forbidden-band zones 211 and 212, and a branch waveguide 25 extending along the direction inclined by −30 degrees. A ray of light within the multiplexed/demultiplexed wavelength band, which is excluded from the transmission wavelength band of the trunk waveguide 24 in the forbidden band zone 212 and included in the transmission wavelength band of the trunk waveguide 24 in the forbidden band zone 211, is reflected by the boundary 23 and thereby demultiplexed from the trunk waveguide 24 into the branch waveguide 25. Thus, all the rays of light whose wavelengths are within the multiplexed/demultiplexed wavelength band having a certain width are demultiplexed into the branch waveguide 25. Therefore, even if the wavelength of the optical signal is deviated due to some error, the light can be demultiplexed. This is also true for the multiplexing operation.
    • 本发明是为了提供能够在具有一定宽度的波长带内复用或分离光的光子晶体。 它包括设置有多个禁带区211和212的板状主体21,并且具有不同尺寸的孔221和222分别布置在不同周期的禁带区中。 还形成有从沿禁带区211和212之间的边界23的垂直方向倾斜+30度的方向延伸的主干波导24和沿着倾斜-30度的方向延伸的分支波导25。 在禁带区域212中被包含在主干波导24的传输波长带中的禁带区域211中从干线波导24的传输波长带排除的复用/解复用波长带内的光线, 由边界23反射,从而从主干波导24分离成分支波导25.因此,波长在具有一定宽度的复用/解复用波长带内的所有光线被解复用到分支波导25中。因此 即使光信号的波长由于一些误差而偏离,也可以将光解复用。 这对于多路复用操作也是如此。
    • 12. 发明授权
    • Two-dimensional photonic crystal
    • 二维光子晶体
    • US07853111B2
    • 2010-12-14
    • US10591299
    • 2005-03-04
    • Susumu NodaTakashi AsanoSeiichi TakayamaHitoshi Kitagawa
    • Susumu NodaTakashi AsanoSeiichi TakayamaHitoshi Kitagawa
    • G02B6/10
    • B82Y20/00G02B6/1225G02B6/29325G02B6/2938
    • The present invention provides a two-dimensional photonic crystal in which an absolute photonic band gap (PBG), i.e. a photonic band gap that is effective for both the TE-polarized light and the TM-polarized light within a predetermined wavelength range, is created with an adequate bandwidth. The body 21 is provided with holes 22 arranged in a triangular lattice pattern, where the basic shape of the hole is an equilateral triangle. This shaping and arranging of the holes creates an absolute PBG. Each corner of the equilateral triangle is cut along an arc to leave an adequate distance between the neighboring holes (i.e. an adequate width of the connecting portion of the body). This design makes it possible to enlarge each hole 22 while ensuring an adequate strength of the two-dimensional photonic crystal. This construction creates an absolute PBG having a large width.
    • 本发明提供一种二维光子晶体,其中产生绝对光子带隙(PBG),即对预定波长范围内的TE偏振光和TM偏振光有效的光子带隙, 具有足够的带宽。 主体21设置有以三角形格子图案布置的孔22,其中孔的基本形状为等边三角形。 这种孔的形成和排列创建了绝对的PBG。 等边三角形的每个角都沿弧线切割,以在相邻的孔之间留下足够的距离(即,身体的连接部分的适当宽度)。 该设计使得可以在确保二维光子晶体的足够强度的同时放大每个孔22。 这种结构创建了宽度大的绝对PBG。
    • 13. 发明授权
    • Photonic crystal having heterostructure and optical device using the photonic crystal
    • 具有异质结构的光子晶体和使用光子晶体的光学器件
    • US07738749B2
    • 2010-06-15
    • US10584942
    • 2005-03-24
    • Susumu NodaTakashi AsanoSeiichi Takayama
    • Susumu NodaTakashi AsanoSeiichi Takayama
    • G02B6/28G02B6/26G02B6/42G02B6/032
    • B82Y20/00G02B6/12004G02B6/1225
    • The present invention has been made for providing a photonic crystal capable of multiplexing or demultiplexing light within a wavelength band having a certain width. It includes a slab-shaped body 21 provided with plural forbidden band zones 211 and 212, and holes 221 and 222 having different sizes are arranged in the forbidden band zones with different cycles, respectively. Also formed are a trunk waveguide 24 extending along the direction inclined by +30 degrees from a perpendicular of the boundary 23 between the forbidden band zones 211 and 212, and a branch waveguide 25 extending along the direction inclined by −30 degrees. A ray of light within the multiplexed/demultiplexed wavelength band, which is excluded from the transmission wavelength band of the trunk waveguide 24 in the forbidden band zone 212 and included in the transmission wavelength band of the trunk waveguide 24 in the forbidden band zone 211, is reflected by the boundary 23 and thereby demultiplexed from the trunk waveguide 24 into the branch waveguide 25. Thus, all the rays of light whose wavelengths are within the multiplexed/demultiplexed wavelength band having a certain width are demultiplexed into the branch waveguide 25. Therefore, even if the wavelength of the optical signal is deviated due to some error, the light can be demultiplexed. This is also true for the multiplexing operation.
    • 本发明是为了提供能够在具有一定宽度的波长带内复用或分离光的光子晶体。 它包括设置有多个禁带区211和212的板状主体21,并且具有不同尺寸的孔221和222分别布置在不同周期的禁带区中。 还形成有沿着从禁带区211和212之间的边界23的垂直方向倾斜±30度的方向延伸的主干波导24和沿着倾斜-30度的方向延伸的分支波导25。 在禁带区域212中被包含在主干波导24的传输波长带中的禁带区域211中从干线波导24的传输波长带排除的复用/解复用波长带内的光线, 由边界23反射,从而从主干波导24分离成分支波导25.因此,波长在具有一定宽度的复用/解复用波长带内的所有光线被解复用到分支波导25中。因此 即使光信号的波长由于一些误差而偏离,也可以将光解复用。 这对于多路复用操作也是如此。
    • 14. 发明授权
    • Two-dimensional photonic crystal and optical device using the crystal
    • 二维光子晶体和使用晶体的光学器件
    • US07711228B2
    • 2010-05-04
    • US11661232
    • 2005-08-30
    • Susumu NodaTakashi AsanoHitoshi KitagawaSeiichi Takayama
    • Susumu NodaTakashi AsanoHitoshi KitagawaSeiichi Takayama
    • G02B6/10
    • G02B6/1225B82Y20/00
    • The present invention intends to provide a two-dimensional photonic crystal having a wide photonic band gap (PBG). In a slab-shaped body 31, a number of holes 32, whose sectional shape on a plane parallel to the slab surface is an equilateral triangle, are periodically arranged in a triangular lattice pattern. The upper and lower sides of the holes 32 are covered with the material of the body 31. The aforementioned sectional shape is uneven along the direction perpendicular to the slab surface. This construction expands the PBG for TM-polarized light and thereby increases its energy region overlapping with the PBG for TE-polarized light. This overlapping section is the complete PBG. If a ray of light whose wavelength corresponds to an energy level within the complete PBG, neither the TE-polarized nor TM-polarized component of the light can be propagated through the photonic crystal. Therefore, even if a waveguide and/or a resonator is provided in the photonic crystal, the light having the aforementioned wavelength will never leak from the waveguide or resonator into the photonic crystal.
    • 本发明旨在提供具有宽光子带隙(PBG)的二维光子晶体。 在板状主体31中,在与平板面平行的平面上的截面形状为等边三角形的多个孔32周期性地排列成三角形格子状。 孔32的上侧和下侧被主体31的材料覆盖。上述截面形状沿着与板坯表面垂直的方向不均匀。 这种结构扩展了TM偏振光的PBG,从而增加了其与TE偏振光的PBG重叠的能量区域。 这个重叠部分是完整的PBG。 如果其波长对应于完整PBG内的能级的光线,则光的TE偏振和TM偏振分量都不能通过光子晶体传播。 因此,即使在光子晶体中设置波导和/或谐振器,具有上述波长的光也不会从波导或谐振器泄漏到光子晶体中。
    • 15. 发明申请
    • Two-Dimensional Photonic Crystal and Optical Device Using the Crystal
    • 二维光子晶体和使用晶体的光学器件
    • US20080013902A1
    • 2008-01-17
    • US11661232
    • 2005-08-30
    • Susumu NodaTakashi AsanoHitoshi KitagawaSeiichi Takayama
    • Susumu NodaTakashi AsanoHitoshi KitagawaSeiichi Takayama
    • G02B6/02G02B6/10
    • G02B6/1225B82Y20/00
    • The present invention intends to provide a two-dimensional photonic crystal having a wide photonic band gap (PBG). In a slab-shaped body 31, a number of holes 32, whose sectional shape on a plane parallel to the slab surface is an equilateral triangle, are periodically arranged in a triangular lattice pattern. The upper and lower sides of the holes 32 are covered with the material of the body 31. The aforementioned sectional shape is uneven along the direction perpendicular to the slab surface. This construction expands the PBG for TM-polarized light and thereby increases its energy region overlapping with the PBG for TE-polarized light. This overlapping section is the complete PBG. If a ray of light whose wavelength corresponds to an energy level within the complete PBG, neither the TE-polarized nor TM-polarized component of the light can be propagated through the photonic crystal. Therefore, even if a waveguide and/or a resonator is provided in the photonic crystal, the light having the aforementioned wavelength will never leak from the waveguide or resonator into the photonic crystal.
    • 本发明旨在提供具有宽光子带隙(PBG)的二维光子晶体。 在板状主体31中,在与平板面平行的平面上的截面形状为等边三角形的多个孔32周期性地排列成三角形格子状。 孔32的上侧和下侧被主体31的材料覆盖。 上述截面形状沿与板坯表面垂直的方向不均匀。 这种结构扩展了TM偏振光的PBG,从而增加了其与TE偏振光的PBG重叠的能量区域。 这个重叠部分是完整的PBG。 如果其波长对应于完整PBG内的能级的光线,则光的TE偏振和TM偏振分量都不能通过光子晶体传播。 因此,即使在光子晶体中设置波导和/或谐振器,具有上述波长的光也不会从波导或谐振器泄漏到光子晶体中。
    • 16. 发明申请
    • Polarized Light Mode Converter
    • 极化光模式转换器
    • US20090232441A1
    • 2009-09-17
    • US11886502
    • 2006-03-07
    • Susumu NodaTakashi AsanoYoshinori TanakaSeiichi Takayama
    • Susumu NodaTakashi AsanoYoshinori TanakaSeiichi Takayama
    • G02B6/00
    • B82Y20/00G02B6/1225G02B6/126G02B6/14
    • The present invention provides a polarized light mode converter which can be provided within a two-dimensional photonic crystal or can be smoothly connected to a two-dimensional photonic crystal. In a two-dimensional photonic crystal made of a slab-like main body provided with a plurality of different refractive index regions (for example, holes 22) arranged in a lattice in the main body, where the different refractive index regions have a refractive index different from that of the main body, a polarized light conversion waveguide 23 is formed which is comprised of defects of the different refractive index regions arranged linearly whose a cross-sectional shape is asymmetrical in a vertical and in a horizontal direction. The polarized light conversion waveguide 23 can be, for example, realized by providing, on a side of the waveguide, holes 221 and 222 extending in a direction oblique to a the main body surface. TE polarized light propagating through the polarized light conversion waveguide 23 is partially converted into TM polarized light due to the asymmetry of the cross-sectional shape of the waveguide. Since the polarized light mode converter is made of a two-dimensional photonic crystal, it can be provided within a two-dimensional photonic crystal or can be smoothly connected to a two-dimensional photonic crystal.
    • 本发明提供一种可以设置在二维光子晶体内或者可以平滑地连接到二维光子晶体的偏振光模式转换器。 在由板状主体构成的二维光子晶体中,其具有在主体中以格子排列的多个不同的折射率区域(例如,孔22),其中不同的折射率区域具有折射率 与主体不同的是,形成偏振光转换波导23,该偏振光转换波导23由横截面形状在垂直方向和水平方向上不对称的直线布置的不同折射率区域的缺陷构成。 例如,偏振光转换波导23可以通过在波导侧设置沿着与主体表面倾斜的方向延伸的孔221和222来实现。 由于波导的横截面形状的不对称性,通过偏振光转换波导23传播的TE偏振光被部分地转换为TM偏振光。 由于偏振光模式转换器由二维光子晶体制成,所以它可以设置在二维光子晶体内,或者可以平滑地连接到二维光子晶体。
    • 17. 发明申请
    • Two-Dimensional Photonic Crystal
    • 二维光子晶体
    • US20080112679A1
    • 2008-05-15
    • US11795991
    • 2006-01-31
    • Susumu NodaTakashi AsanoSeiichi TakayamaRanko Hatsuda
    • Susumu NodaTakashi AsanoSeiichi TakayamaRanko Hatsuda
    • G02B6/10
    • B82Y20/00G02B6/1225
    • An objective of the present invention is to provide a two-dimensional photonic crystal in which a complete photonic band gap (PBG), i.e. a photonic band gap that is effective for both a TE-polarized light and a TM-polarized light within a predetermined wavelength range, is created and an adequate width of the complete PBG can be ensured. A slab-shaped body 21 consisting of a birefringent material is provided with holes 22 periodically arranged in a triangular lattice pattern, where a plane shape of the hole is an equilateral triangle. The PBG for the TE-polarized light and the PBG for the TM-polarized light can be independently set by adjusting anisotropy in the refractive index of the body 21, i.e. a refractive index in a direction vertical to the body 21 and a refractive index in a direction parallel to the body 21. This construction makes it possible to ensure an adequate width of the complete PBG.
    • 本发明的目的是提供一种二维光子晶体,其中完整的光子带隙(PBG),即对预定的TE偏振光和TM偏振光两者都有效的光子带隙 波长范围,并且可以确保完整PBG的足够宽度。 由双折射材料构成的板状体21设置有以三角形格子图案周期性排列的孔22,孔的平面形状为等边三角形。 用于TE偏振光的PBG和用于TM偏振光的PBG可以通过调节主体21的折射率的各向异性,即垂直于主体21的方向上的折射率和折射率,独立地设定 平行于主体21的方向。这种结构使得可以确保完整的PBG的宽度。
    • 18. 发明授权
    • Light-emitting device and organic electroluminescence light-emitting device
    • 发光元件及有机电致发光元件
    • US08704253B2
    • 2014-04-22
    • US10550653
    • 2004-03-19
    • Susumu NodaTakashi AsanoMasayuki FujitaHiroshi Ohata
    • Susumu NodaTakashi AsanoMasayuki FujitaHiroshi Ohata
    • H01L33/00
    • H01L51/5275H01L51/0035H01L51/0036H01L51/0037H01L51/0038H01L51/0051H01L51/0052H01L51/0059H01L51/007H01L51/5262
    • In conventional organic EL light-emitting devices, the ITO used for a transparent electrode has a refractive index of about 2.0 larger than the refractive index of 1.5 of a transparent glass substrate. As a result, the mode of most of light traveling from the transparent electrode toward the glass substrate is the transparent electrode guided mode, and no light is emitted from the transparent electrode toward the glass substrate. According to the invention, the light extraction efficiency of conventional light-emitting devices such as organic EL light-emitting devices is improved by using mode conversion means so as to solve the problem that conventional light-emitting devices such as organic EL light-emitting devices have low light extraction efficiencies. A light-emitting device of the invention comprises a light-emitting layer on a substrate and mode conversion means for converting the mode from the guided mode into an emission mode. The mode conversion means is provided in the substrate, in the light-emitting layer, or at the interface between the substrate and the light-emitting layer.
    • 在传统的有机EL发光器件中,用于透明电极的ITO具有比透明玻璃衬底的折射率1.5大约2.0的折射率。 结果,从透明电极朝向玻璃基板行进的大部分光的模式是透明电极引导模式,并且没有光从透明电极朝向玻璃基板发射。 根据本发明,通过使用模式转换装置来提高诸如有机EL发光器件的常规发光装置的光提取效率,以解决诸如有机EL发光装置之类​​的常规发光装置的问题 具有低光提取效率。 本发明的发光装置包括在基板上的发光层和用于将模式从导模转换为发射模式的模式转换装置。 模式转换装置设置在基板,发光层中或基板与发光层之间的界面处。
    • 19. 发明授权
    • Two-dimensional photonic crystal optical multiplexer/demultiplexer
    • 二维光子晶体光复用器/解复用器
    • US07590325B2
    • 2009-09-15
    • US10507889
    • 2003-03-26
    • Susumu NodaMasamitu MochizukiTakashi Asano
    • Susumu NodaMasamitu MochizukiTakashi Asano
    • G02B6/10
    • G02B6/1225B82Y20/00
    • The present invention provides an optical multiplexer/demultiplexer that can be smaller in size and higher in Q-factor or efficiency. This object is achieved by the following construction. In a slab-shaped body 11, low refractive index areas 12 having a refractive index lower than that of the material of the body 11 are periodically arranged to construct a two-dimensional photonic crystal, in which a waveguide 13 is formed by not boring holes 12 linearly. A donor type cluster defect 14 is formed by not boring holes 12 at two ore more lattice points located adjacent to the waveguide 13. With this construction, only a specific wavelength of light included in the light propagating through the waveguide 13 resonates at the donor type cluster 14, and the light thus trapped is released to the outside (demultiplexing). Conversely, only a specific wavelength of light may be introduced through the donor type cluster defect 14 into the waveguide 13 (multiplexing).
    • 本发明提供了一种光复用器/解复用器,其尺寸可以更小并且Q因子或效率更高。 该目的通过以下结构实现。 在板状体11中,周期性地布置折射率低于主体11的折射率的低折射率区域12,以构成二维光子晶体,其中通过不钻孔形成波导13 12线性。 供体型簇缺陷14通过在与波导13相邻的两个多个晶格点处不钻孔12而形成。利用这种结构,包含在通过波导13传播的光中的特定波长的光在施主型 簇14,并且被捕获的光被释放到外部(解复用)。 相反,只有特定波长的光可以通过供体型簇缺陷14引入波导13(复用)。
    • 20. 发明授权
    • Two-dimensional photonic crystal slab having three-dimensional local structure
    • 具有三维局部结构的二维光子晶体板
    • US07397994B2
    • 2008-07-08
    • US10537119
    • 2003-12-05
    • Susumu NodaTakashi AsanoYoshinori Tanaka
    • Susumu NodaTakashi AsanoYoshinori Tanaka
    • G02B6/10
    • B82Y20/00G02B6/12002G02B6/1225G02F2202/32
    • The present invention aims to provide a two-dimensional photonic crystal having an optical resonator, which allows the control of the front/back emission ratio of light. To achieve this object, a refractive index member made of a material having a refractive index different from that of air is mounted on a two-dimensional photonic crystal having a body in which holes are periodically arranged. In this construction, the body and the refractive index member cooperatively function as an optical resonator located at the position where the refractive index member is mounted. The light emitted from this optical resonator is stronger on the side having a higher refractive index, i.e. on the side where the refractive index member is mounted. Accordingly, the light emitted from the side where the refractive index member is mounted is stronger than the light emitted from the other side. The ratio of the emission intensity of the two rays of light and, i.e. the front/back emission ratio, can be controlled by changing the material, shape and/or size of the refractive index member.
    • 本发明旨在提供一种具有光谐振器的二维光子晶体,其允许控制光的前/后发射比。 为了实现该目的,由具有与空气的折射率不同的折射率的材料制成的折射率构件安装在具有周期性布置有孔的主体的二维光子晶体上。 在这种结构中,主体和折射率构件协调地用作位于折射率构件安装位置的光学谐振器。 从该光谐振器发射的光在具有较高折射率的一侧,即在折射率构件安装的一侧更强。 因此,从安装有折射率构件的一侧发射的光比从另一侧发射的光更强。 可以通过改变折射率构件的材料,形状和/或尺寸来控制两束光的发射强度的比例,即前/后发射比。