公开(公告)号：US06903549B2

公开(公告)日：2005-06-07

申请号：US10362181

申请日：2001-08-08

Applicant: Hans W. P. Koops ,  Alexander Kaya

Inventor： Hans W. P. Koops ,  Alexander Kaya

IPC: H01J49/06 ,  H01J49/44 ,  H01J49/48 ,  H01L29/06 ,  H01L29/76 ,  G01V3/00

CPC classification number: B82Y10/00 ,  H01J49/44 ,  H01L29/7613

Abstract: Inordinate localised systems are used at room temperature in a novel device in the form of an electron spectrometer for utilising single-electron electronic applications. Said electron spectrometer device consists of a nanocrystalline metal or a nanocrystalline semiconductor material used as conductor strip connection in the form of an inlet or an outlet for single-electron electronic components and circuits consisting of lithographically produced quantum dots. The resulting single-electron electronic device consisting of quantum dots is supplied with energetically very sharply defined electrons. Said device can thus be operated at room temperature, undisturbed by phonons.

Abstract translation: 在室温下使用过量的局部化系统以电子光谱仪形式用于利用单电子电子应用的新型器件。 所述电子分光计装置由纳米晶体金属或纳米晶体半导体材料组成，该材料用作单晶电子元件入口或出口形式的导体条连接，以及由光刻产生的量子点组成的电路。 所产生的由量子点组成的单电子电子器件被提供能量非常清晰的电子。 因此，所述装置可以在室温下操作，而不被声子干扰。

公开(公告)号：US06967714B2

公开(公告)日：2005-11-22

申请号：US10240221

申请日：2001-03-24

Applicant: Hans W. P. Koops ,  Alexander Kaya ,  Ottokar Leminger

Inventor： Hans W. P. Koops ,  Alexander Kaya ,  Ottokar Leminger

IPC: G01N21/41 ,  G01N21/47

CPC classification number: G01N21/4788 ,  G01N21/41

Abstract: The matter for which the refractive index is to be determined, is made available in the form of a theoretically determinable scattering or diffraction pattern. Two or more orders of diffraction may then be defined to form at least one intensity ratio. At least one intensity distribution may be formed by irradiating the scattering pattern using one light beam of a defined shape. Subsequently thereto, the intensity ratio may be formed based on the orders of diffraction of the intensity distribution. In addition, at least one portion of a characteristic curve may be determined, which represents the dependency of the intensity ratio on the refractive index, and, with whose assistance, the corresponding refractive index can be assigned to the intensity ratio formed.

Abstract translation: 要确定折射率的问题以理论上可确定的散射或衍射图案的形式提供。 然后可以限定两个或多个衍射级以形成至少一个强度比。 可以通过使用具有限定形状的一个光束照射散射图案来形成至少一个强度分布。 随后，可以基于强度分布的衍射次数来形成强度比。 此外，可以确定特征曲线的至少一部分，其表示强度比对折射率的依赖性，并且通过它们的帮助可以将相应的折射率分配给所形成的强度比。

公开(公告)号：US07435973B2

公开(公告)日：2008-10-14

申请号：US11499776

申请日：2006-08-07

Applicant: Hans W. P. Koops ,  Peter Hoffrogge

Inventor： Hans W. P. Koops ,  Peter Hoffrogge

IPC: G21K7/00

CPC classification number: H01J37/3056 ,  H01J2237/006 ,  H01J2237/162 ,  H01J2237/166 ,  H01J2237/31732 ,  H01J2237/31744

Abstract: A material processing system for processing a work piece is provided. The material processing is effected by supplying a reactive gas and energetic radiation for activation of the reactive gas to a surrounding of a location of the work piece to be processed. The radiation is preferably provided by an electron microscope. An objective lens of the electron microscope is preferably disposed between a detector of the electron microscope and the work piece. A gas supply arrangement of the material processing system comprises a valve disposed spaced apart from the processing location, a gas volume between the valve and a location of emergence of the reaction gas being small. The gas supply arrangement further comprises a temperature-adjusted, especially cooled reservoir for accommodating a starting material for the reactive gas.

Abstract translation: 提供了一种用于处理工件的材料处理系统。 材料处理通过提供反应气体和能量辐射来激活反应气体到待处理工件的位置的周围。 辐射优选由电子显微镜提供。 电子显微镜的物镜优选设置在电子显微镜的检测器和工件之间。 材料处理系统的气体供应装置包括与处理位置间隔开的阀，阀之间的气体体积和反应气体的出现位置较小。 气体供应装置还包括温度调节的特别冷却的储存器，用于容纳用于反应气体的起始材料。

公开(公告)号：US6075915A

公开(公告)日：2000-06-13

申请号：US048508

申请日：1998-03-26

Applicant: Hans W. P. Koops ,  Gerald Meltz

Inventor： Hans W. P. Koops ,  Gerald Meltz

IPC: G02B6/12 ,  G02B6/02 ,  G02B6/122 ,  G02F1/01 ,  G02F1/365 ,  G02F1/377 ,  G02B6/20

CPC classification number: G02B6/02309 ,  B82Y20/00 ,  G02B6/1225 ,  G02F2202/32

Abstract: One or more photonic crystals 11, 22, 40, 58, 59 are formed directly in the path of light within an optical fiber 13, 23, 42, 56. Light processed by the photonic crystal may be transmitted out of the fiber by means of a lens 48 or it may be measured by a photoresistive device 51, 60. The photonic crystal may be formed in a trench 12 as an array of dielectric rods 16 having one or more selective defects 17, or the crystal may be formed by providing holes 20 directly in the optical fiber. Filling the interstices between rods 16 with non-linear optical material, and subjecting the crystal to a varying electric field applied by electrodes or to a varying optical radiation can produce a tunable photonic crystal within an optical fiber.

Abstract translation: 一个或多个光子晶体11,22,40,58,59直接形成在光纤13,23,42和56内的光路中。由光子晶体处理的光可以通过 透镜48或其可以由光致抗蚀剂装置51,60测量。光子晶体可以形成为具有一个或多个选择性缺陷17的介电棒16的阵列的沟槽12，或者可以通过提供孔形成晶体 20直接在光纤中。 用非线性光学材料填充杆16之间的间隙，以及使晶体经受由电极或变化的光辐射施加的变化的电场，可在光纤内产生可调光子晶体。

公开(公告)号：US08648319B2

公开(公告)日：2014-02-11

申请号：US13812213

申请日：2011-07-26

Applicant: Hans W. P. Koops

Inventor： Hans W. P. Koops

IPC: H01S5/183 ,  H01S5/026 ,  H01S3/00 ,  G02F1/00

CPC classification number: B01J19/128 ,  H01J25/68 ,  H01J25/76 ,  H03B2200/0084

Abstract: The invention relates to a device for generating electromagnetic THz radiation with free electron beams, comprising a dynatron tube, where the dynatron tube comprises an electron source, an extraction grid, and, an anode preferably coated with a material composition for high secondary electron emission, arranged in vacuum. The dynatron tube is connected to a voltage supply supplying an extractor voltage and an anode voltage and the extractor voltage is higher than the anode voltage. An oscillator modulates the anode voltage and the anode voltage is set to a work point voltage.

Abstract translation: 本发明涉及一种用于产生具有自由电子束的电磁THz辐射的装置，其包括一个放电管，其中该电子管包括一个电子源，一个提取栅格，以及一个优选涂覆有用于高二次电子发射的材料组合物的阳极， 排列在真空中。 电极管连接到提供提取器电压和阳极电压的电压源，并且提取器电压高于阳极电压。 振荡器调制阳极电压，阳极电压设定为工作点电压。

公开(公告)号：US08868156B1

公开(公告)日：2014-10-21

申请号：US10149045

申请日：2000-11-22

Applicant: Hans W. P. Koops ,  Andreas Reinhardt

Inventor： Hans W. P. Koops ,  Andreas Reinhardt

IPC: A61B5/00

CPC classification number: G01N21/6452 ,  G01J3/02 ,  G01J3/0256 ,  G01J3/0259 ,  G01J3/4406 ,  G01J3/443 ,  G01N2021/6417 ,  G01N2021/6478

Abstract: A device (1) for use in optical spectroscopy and a method for its manufacture are described. The device includes at least one light source (8) and at least one spectrometer (3) fabricated integratively, the optical components of the at least one spectrometer (3) being optical microcomponents (11,13,16,19,20,21) which are mounted integratively on the top and/or bottom side (9,12) of a substrate board (2). In the method according to the present invention, at least one light source (8) is mounted on a substrate board (2), and at least one spectrometer (3) is produced monolithically in a three-dimensional integration on the substrate board (2). In this context, the spectrometer (3) that is produced according to the method is assembled from optical microcomponents (11,13,16,19,20,21).

Abstract translation: 描述了用于光谱学的装置（1）及其制造方法。 所述装置包括至少一个光源（8）和至少一个光谱仪（3），所述至少一个光谱仪（3）被整体地制造，所述至少一个光谱仪（3）的光学部件是光学微组件（11,13,16,19,20,21） 它们一体地安装在基板（2）的顶部和/或底部（9,12）上。 在根据本发明的方法中，至少一个光源（8）安装在基板（2）上，并且至少一个光谱仪（3）在基板（2）上以三维积分制造 ）。 在本文中，根据该方法制备的光谱仪（3）由光学微组件（11,13,16,19,20,21）组装。

公开(公告)号：US06760513B1

公开(公告)日：2004-07-06

申请号：US09937579

申请日：2001-12-20

Applicant: Walter Heitmann ,  Hans W. P. Koops

Inventor： Walter Heitmann ,  Hans W. P. Koops

IPC: G02B634

CPC classification number: G02B6/29394 ,  B82Y20/00 ,  G02B6/12007 ,  G02B6/1225 ,  H04B10/25133

Abstract: The present invention is directed to an economical approach for compensating for the dispersion of optical signals having different wavelengths. In accordance with the present invention, photonic crystals (K1-Kn) are positioned on a common optical waveguide (2). In this context, each photonic crystal (K1-Kn) is tuned to reflect or deflect the signals of one wavelength and to transmit the signals of other wavelengths, unattenuated. The specific arrangement of the photonic crystals (K1-Kn) on the waveguide (2) and the specific arrangement of the deflecting elements in the photonic crystal are defined, in the process, as a function of the dispersion to be compensated for between the individual wavelengths. The approach of the present invention makes it possible to assemble permanently set or controllable photonic dispersion compensators of a high quality, which are approximately 1000 times shorter than conventional diffraction gratings.

Abstract translation: 本发明涉及用于补偿具有不同波长的光信号的色散的经济方法。根据本发明，光子晶体（K1-Kn）位于公共光波导（2）上。 在这种情况下，每个光子晶体（K1-Kn）被调谐以反射或偏转一个波长的信号并且传输其它波长的信号，而不是衰减的。 光子晶体（K1-Kn）在波导（2）上的具体布置以及光子晶体中的偏转元件的具体布置被定义为在该过程中作为待个体之间补偿的色散的函数 本发明的方法使得可以组装高质量的永久设置或可控的光子色散补偿器，其比常规衍射光栅近约1000倍。

公开(公告)号：US6093246A

公开(公告)日：2000-07-25

申请号：US574810

申请日：1995-12-19

Applicant: Shawn-Yu Lin ,  Hans W. P. Koops

Inventor： Shawn-Yu Lin ,  Hans W. P. Koops

IPC: G02B6/122 ,  G02B6/13 ,  G02B6/132 ,  G03F7/00 ,  C30B29/02

CPC classification number: B82Y20/00 ,  G02B6/1221 ,  G02B6/1225 ,  G02B6/13 ,  G02B6/132 ,  G03F7/001

Abstract: A photonic crystal device and method. The photonic crystal device comprises a substrate with at least one photonic crystal formed thereon by a charged-particle beam deposition method. Each photonic crystal comprises a plurality of spaced elements having a composition different from the substrate, and may further include one or more impurity elements substituted for spaced elements. Embodiments of the present invention may be provided as electromagnetic wave filters, polarizers, resonators, sources, mirrors, beam directors and antennas for use at wavelengths in the range from about 0.2 to 200 microns or longer. Additionally, photonic crystal devices may be provided with one or more electromagnetic waveguides adjacent to a photonic crystal for forming integrated electromagnetic circuits for use at optical, infrared, or millimeter-wave frequencies.

Abstract translation: 一种光子晶体器件及方法。 光子晶体器件包括通过带电粒子束沉积方法在其上形成有至少一个光子晶体的衬底。 每个光子晶体包括具有不同于衬底的组成的多个间隔元件，并且还可包括取代间隔元件的一个或多个杂质元素。 本发明的实施例可以被提供为在约0.2至200微米或更长的波长范围内使用的电磁波滤波器，偏振器，谐振器，源，反射镜，光束导向器和天线。 此外，光子晶体器件可以设置有与光子晶体相邻的一个或多个电磁波导，用于形成用于光学，红外或毫米波频率的集成电磁电路。

公开(公告)号：US5982962A

公开(公告)日：1999-11-09

申请号：US993066

申请日：1997-12-18

Applicant: Hans W. P. Koops ,  Gerald Meltz

Inventor： Hans W. P. Koops ,  Gerald Meltz

IPC: G02B6/32 ,  G01J3/18 ,  G02B6/02 ,  G02B6/34

CPC classification number: G02B6/02057 ,  G01J3/1895 ,  G01J3/0256 ,  G01J3/18 ,  G02B6/29323

Abstract: A microlens 30 is formed on the outer surface of an optical fiber 20 having an in-fiber Bragg grating 24 (FBG) formed in the core 21, 36 thereof, to focus light diffracted by the FBG onto other fibers or optical devices, or to focus light received at the fiber onto the FBG. Various single- and multi-microlens configurations of one or more fibers perform a variety of functions such as signal coupling, multiplexing, signal splitting, spectrography, tapped delay, timed-delay phase adjusting, circulating storage, and so forth. The microlenses may employ angle-increasing prisms and may comprise Fresnel lenses.

Abstract translation: 微型透镜30形成在光纤20的外表面上，该光纤20具有形成在其芯21,36中的光纤内布拉格光栅24（FBG），以将由FBG衍射的光聚焦到其它光纤或光学器件上，或者 将光纤上的聚焦光聚焦到FBG上。 一个或多个光纤的各种单和多微透镜配置执行各种功能，例如信号耦合，复用，信号分离，光谱学，抽头延迟，定时延迟相位调整，循环存储等。 微透镜可以采用增角棱镜，并且可以包括菲涅耳透镜。

公开(公告)号：US20130264500A1

公开(公告)日：2013-10-10

申请号：US13812213

申请日：2011-07-26

Applicant: Hans W. P. Koops

Inventor： Hans W. P. Koops

IPC: B01J19/12

CPC classification number: B01J19/128 ,  H01J25/68 ,  H01J25/76 ,  H03B2200/0084

Abstract: The invention relates to a device for generating electromagnetic THz radiation with free electron beams, comprising a dynatron tube, where the dynatron tube comprises an electron source, an extraction grid, and, an anode preferably coated with a material composition for high secondary electron emission, arranged in vacuum. The dynatron tube is connected to a voltage supply supplying an extractor voltage and an anode voltage and the extractor voltage is higher than the anode voltage. An oscillator modulates the anode voltage and the anode voltage is set to a work point voltage.

Abstract translation: 本发明涉及一种用于产生具有自由电子束的电磁THz辐射的装置，其包括一个放电管，其中该电子管包括一个电子源，一个提取栅格，以及一个优选涂覆有用于高二次电子发射的材料组合物的阳极， 排列在真空中。 电极管连接到提供提取器电压和阳极电压的电压源，并且提取器电压高于阳极电压。 振荡器调制阳极电压，阳极电压设定为工作点电压。