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    • 1. 发明申请
    • Two-dimensional photonic crystal having air-bridge structure and method for manufacturing such a crystal
    • 具有气桥结构的二维光子晶体及其制造方法
    • US20080145012A1
    • 2008-06-19
    • US12004029
    • 2007-12-20
    • Ranko HatsudaSusumu NodaTakashi AsanoYoshinori TanakaEiji Miyai
    • Ranko HatsudaSusumu NodaTakashi AsanoYoshinori TanakaEiji Miyai
    • G02B6/10
    • G02B6/13B82Y20/00G02B6/12004G02B6/12007G02B6/1225
    • The present invention intends to provide a two-dimensional photonic crystal having a high level of mechanical strength and functioning as a high-efficiency resonator. The two-dimensional photonic crystal according to the present invention includes a slab layer 31 under which a clad layer 32 is located. In the slab layer 31, areas 35 having a refractive index different from that of the slab layer 31 are cyclically arranged to create a two-dimensional photonic crystal. A portion of the cyclic arrangement of the areas 35 are omitted to form a point-like defect 36. This defect 36 functions as a resonator at which a specific wavelength of light resonates. An air-bridge cavity 37 facing the point-like defect 36 is formed over a predetermined range of the clad layer 32. In this construction, the clad layer 32 supports the slab layer 31 except for the range over which the air-bridge space 37 is formed. Therefore, the two-dimensional photonic crystal has a high level of mechanical strength. The presence of the air-bridge space 37 under the point-like defect 36 makes it easy to confine light at the point-like defect 36 by the difference in the refractive index between the slab layer 31 and the air. Thus, the point-like defect 36 functions as a high-performance resonator.
    • 本发明旨在提供具有高水平机械强度并用作高效率谐振器的二维光子晶体。 根据本发明的二维光子晶体包括平坦层31,覆层32位于其下方。 在板坯层31中,具有不同于板坯层31的折射率的区域35循环地布置以产生二维光子晶体。 区域35的循环布置的一部分被省略以形成点状缺陷36。 该缺陷36用作特定波长的光谐振的谐振器。 在包层32的预定范围上形成面向点状缺陷36的空气桥腔37。 在这种结构中,除了形成空气桥隔间37的范围之外,包覆层32支撑板层31。 因此,二维光子晶体具有高水平的机械强度。 点状缺陷36之下的空气桥空间37的存在使得容易通过板状层31和空气之间的折射率差来限制点状缺陷36处的光。 因此,点状缺陷36用作高性能谐振器。
    • 2. 发明授权
    • Two-dimensional photonic crystal having air-bridge structure and method for manufacturing such a crystal
    • 具有气桥结构的二维光子晶体及其制造方法
    • US07509014B2
    • 2009-03-24
    • US12004029
    • 2007-12-20
    • Ranko HatsudaSusumu NodaTakashi AsanoYoshinori TanakaEiji Miyai
    • Ranko HatsudaSusumu NodaTakashi AsanoYoshinori TanakaEiji Miyai
    • G02B6/00G02B6/10
    • G02B6/13B82Y20/00G02B6/12004G02B6/12007G02B6/1225
    • The present invention intends to provide a two-dimensional photonic crystal having a high level of mechanical strength and functioning as a high-efficiency resonator. The two-dimensional photonic crystal according to the present invention includes a slab layer 31 under which a clad layer 32 is located. In the slab layer 31, areas 35 having a refractive index different from that of the slab layer 31 are cyclically arranged to create a two-dimensional photonic crystal. A portion of the cyclic arrangement of the areas 35 are omitted to form a point-like defect 36. This defect 36 functions as a resonator at which a specific wavelength of light resonates. An air-bridge cavity 37 facing the point-like defect 36 is formed over a predetermined range of the clad layer 32. In this construction, the clad layer 32 supports the slab layer 31 except for the range over which the air-bridge space 37 is formed. Therefore, the two-dimensional photonic crystal has a high level of mechanical strength. The presence of the air-bridge space 37 under the point-like defect 36 makes it easy to confine light at the point-like defect 36 by the difference in the refractive index between the slab layer 31 and the air. Thus, the point-like defect 36 functions as a high-performance resonator.
    • 本发明旨在提供具有高水平机械强度并用作高效率谐振器的二维光子晶体。 根据本发明的二维光子晶体包括平坦层31,覆层32位于其下方。 在板坯层31中,具有不同于板坯层31的折射率的区域35循环地布置以产生二维光子晶体。 区域35的循环布置的一部分被省略以形成点状缺陷36.该缺陷36用作特定波长的光谐振的谐振器。 在包覆层32的预定范围上形成面向点状缺陷36的空气桥腔37.在该结构中,包覆层32支撑板层31,除了空气桥空间37 形成了。 因此,二维光子晶体具有高水平的机械强度。 点状缺陷36之下的空气桥空间37的存在使得容易通过板状层31和空气之间的折射率差来限制点状缺陷36处的光。 因此,点状缺陷36用作高性能谐振器。
    • 3. 发明授权
    • Two-dimensional photonic crystal having air-bridge structure and method for manufacturing such a crystal
    • 具有气桥结构的二维光子晶体及其制造方法
    • US07333703B2
    • 2008-02-19
    • US10569879
    • 2004-08-27
    • Ranko HatsudaSusumu NodaTakashi AsanoYoshinori TanakaEiji Miyai
    • Ranko HatsudaSusumu NodaTakashi AsanoYoshinori TanakaEiji Miyai
    • G02B6/10C03B37/023C03B37/022C03B37/027
    • G02B6/13B82Y20/00G02B6/12004G02B6/12007G02B6/1225
    • The present invention intends to provide a two-dimensional photonic crystal having a high level of mechanical strength and functioning as a high-efficiency resonator. The two-dimensional photonic crystal according to the present invention includes a slab layer 31 under which a clad layer 32 is located. In the slab layer 31, areas 35 having a refractive index different from that of the slab layer 31 are cyclically arranged to create a two-dimensional photonic crystal. A portion of the cyclic arrangement of the areas 35 are omitted to form a point-like defect 36. This defect 36 functions as a resonator at which a specific wavelength of light resonates. An air-bridge cavity 37 facing the point-like defect 36 is formed over a predetermined range of the clad layer 32. In this construction, the clad layer 32 supports the slab layer 31 except for the range over which the air-bridge space 37 is formed. Therefore, the two-dimensional photonic crystal has a high level of mechanical strength. The presence of the air-bridge space 37 under the point-like defect 36 makes it easy to confine light at the point-like defect 36 by the difference in the refractive index between the slab layer 31 and the air. Thus, the point-like defect 36 functions as a high-performance resonator.
    • 本发明旨在提供具有高水平机械强度并用作高效率谐振器的二维光子晶体。 根据本发明的二维光子晶体包括平坦层31,覆层32位于其下方。 在板坯层31中,具有不同于板坯层31的折射率的区域35循环地布置以产生二维光子晶体。 区域35的循环布置的一部分被省略以形成点状缺陷36.该缺陷36用作特定波长的光谐振的谐振器。 在包覆层32的预定范围上形成面向点状缺陷36的空气桥腔37.在该结构中,包覆层32支撑板层31,除了空气桥空间37 形成了。 因此,二维光子晶体具有高水平的机械强度。 点状缺陷36之下的空气桥空间37的存在使得容易通过板状层31和空气之间的折射率差来限制点状缺陷36处的光。 因此,点状缺陷36用作高性能谐振器。
    • 4. 发明申请
    • Two-dimensional photonic crystal having air-bridge structure and method for manufacturing such a crystal
    • 具有气桥结构的二维光子晶体及其制造方法
    • US20070009219A1
    • 2007-01-11
    • US10569879
    • 2004-08-27
    • Ranko HatsudaSusumu NodaTakashi AsanoYoshinori TanakaEiji Miyai
    • Ranko HatsudaSusumu NodaTakashi AsanoYoshinori TanakaEiji Miyai
    • G02B6/10
    • G02B6/13B82Y20/00G02B6/12004G02B6/12007G02B6/1225
    • The present invention intends to provide a two-dimensional photonic crystal having a high level of mechanical strength and functioning as a high-efficiency resonator. The two-dimensional photonic crystal according to the present invention includes a slab layer 31 under which a clad layer 32 is located. In the slab layer 31, areas 35 having a refractive index different from that of the slab layer 31 are cyclically arranged to create a two-dimensional photonic crystal. A portion of the cyclic arrangement of the areas 35 are omitted to form a point-like defect 36. This defect 36 functions as a resonator at which a specific wavelength of light resonates. An air-bridge cavity 37 facing the point-like defect 36 is formed over a predetermined range of the clad layer 32. In this construction, the clad layer 32 supports the slab layer 31 except for the range over which the air-bridge space 37 is formed. Therefore, the two-dimensional photonic crystal has a high level of mechanical strength. The presence of the air-bridge space 37 under the point-like defect 36 makes it easy to confine light at the point-like defect 36 by the difference in the refractive index between the slab layer 31 and the air. Thus, the point-like defect 36 functions as a high-performance resonator.
    • 本发明旨在提供具有高水平机械强度并用作高效率谐振器的二维光子晶体。 根据本发明的二维光子晶体包括平坦层31,覆层32位于其下方。 在板坯层31中,具有不同于板坯层31的折射率的区域35循环地布置以产生二维光子晶体。 区域35的循环布置的一部分被省略以形成点状缺陷36.该缺陷36用作特定波长的光谐振的谐振器。 在包覆层32的预定范围上形成面向点状缺陷36的空气桥腔37.在该结构中,包覆层32支撑板层31,除了空气桥空间37 形成了。 因此,二维光子晶体具有高水平的机械强度。 点状缺陷36之下的空气桥空间37的存在使得容易通过板状层31和空气之间的折射率差来限制点状缺陷36处的光。 因此,点状缺陷36用作高性能谐振器。
    • 5. 发明授权
    • Two-dimensional photonic crystal
    • 二维光子晶体
    • US07509013B2
    • 2009-03-24
    • 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。
    • 6. 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。
    • 7. 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。
    • 8. 发明申请
    • Two-dimensional photonic crystal slab having local tree-dimensional structure
    • 具有局部树维结构的二维光子晶体板
    • US20060051042A1
    • 2006-03-09
    • 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 (13) made of a material having a refractive index different from that of air is mounted on a two-dimensional photonic crystal having a body (11) in which holes (12) are periodically arranged. In this construction, the body (11) and the refractive index member (13) cooperatively function as an optical resonator located at the position where the refractive index member (13) 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 (191) emitted from the side where the refractive index member (13) is mounted is stronger than the light (192) emitted from the other side. The ratio of the emission intensity of the two rays of light (191) and (192), 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。 为了实现这个目的,由具有不同于空气的折射率的材料制成的折射率构件(13)安装在具有周期性布置有孔(12)的主体(11)的二维光子晶体上。 在这种结构中,主体(11)和折射率构件(13)协调地用作位于折射率构件(13)的位置处的光学谐振器。 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,从折射率构件(13)安装的一侧发射的光(191)比从另一侧发射的光(192)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(191)和(192)的发射强度的比率,即前/后发射比。
    • 9. 发明申请
    • POLARIZATION-INDEPENDENT TWO-DIMENSIONAL PHOTONIC CRYSTAL MULTIPLEXER/DEMULTIPLEXER
    • 极化独立二维光子晶体多路复用器/解复用器
    • US20090162008A1
    • 2009-06-25
    • US12438491
    • 2007-08-27
    • Susumu NodaTakashi AsanoYoshinori Tanaka
    • Susumu NodaTakashi AsanoYoshinori Tanaka
    • G02B6/12
    • G02B6/1225B82Y20/00G02B6/12007G02B6/126G02B2006/12147G02B2006/1215G02B2006/12164
    • The present invention is aimed at providing a two-dimensional photonic crystal wavelength multiplexer/demultiplexer capable of multiplexing and demultiplexing both TE and TM-polarized lights. In the wavelength multiplexer/demultiplexer, first and second resonators and having the same resonance wavelength λr are provided between first and second waveguides and which are separately provided in a two-dimensional photonic crystal having a photonic band gap for the TE polarization. A first polarization converter for converting a TM-polarized light to a TE-polarized light is provided on the first waveguide 121 between the first and second resonators and. Similarly, a second polarization converter for converting a TE-polarized light to a TM-polarized light is provided on the second waveguide between the first and second resonators and. Among the light propagating through the first waveguide, the TE-polarized light with wavelength λr is introduced from the first resonator into the second waveguide, whereas the TM-polarized light is converted to a TE-polarized light by the first polarization converter and then introduced through the second resonator into the second waveguide.
    • 本发明旨在提供一种能够对TE和TM偏振光进行多路复用和解复用的二维光子晶体波长多路复用器/解复用器。 在波长多路复用器/解复用器中,在第一和第二波导之间提供具有相同谐振波长的第一和第二谐振器,并且分别设置在具有用于TE极化的光子带隙的二维光子晶体中。 用于将TM偏振光转换为TE偏振光的第一偏振转换器设置在第一和第二谐振器之间的第一波导121上。 类似地,在第一和第二谐振器之间的第二波导上提供用于将TE偏振光转换为TM偏振光的第二偏振转换器。 在通过第一波导传播的光中,从第一谐振器引入具有波长兰伯的TE偏振光到第二波导,而通过第一偏振转换器将TM偏振光转换成TE偏振光,然后引入 通过第二谐振器进入第二波导。
    • 10. 发明授权
    • Polarized light mode converter
    • 极化光模式转换器
    • US07783139B2
    • 2010-08-24
    • 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。