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    • 92. 发明申请
    • ELECTRONIC COMPONENT AND PROCESS FOR MAKING IT
    • 电子元件及其制造工艺
    • WO1993013560A1
    • 1993-07-08
    • PCT/DE1992001080
    • 1992-12-19
    • FORSCHUNGSZENTRUM JÜLICH GMBHGRÄBER, Jürgen
    • FORSCHUNGSZENTRUM JÜLICH GMBH
    • H01L29/76
    • H01L29/66454H01L27/0605H01L29/7722Y10S148/011
    • The invention relates to an electronic component with a plurality of layers produced in the combination and with at least one laterally structured layer designed to control a space charge region. In addition, the invention relates to a process for producing such a component. The aim of the invention is such an electronic component having an enhanced switching speed. To this end, the component of the invention has a pn junction as a space charge region with a p and an n conducting layer. One of the two layers is the laterally structured base. Finally, in order to reduce parasitic space charge capacitances in the region of the lateral boundary surfaces, particularly not designed to control the space charge region at the base, the component has an additional layer having the same lateral structure at one of the two lateral boundary surfaces of the base.
    • 本发明涉及一种电子部件,其具有以组合形式产生的多个层,以及设计成控制空间电荷区域的至少一个侧向结构化层。 此外,本发明涉及一种生产这种组分的方法。 本发明的目的是具有增强的切换速度的电子部件。 为此,本发明的组分具有pn结作为具有p和n导电层的空间电荷区。 两层之一是横向结构化的基座。 最后,为了减少横向边界表面区域中的寄生空间电荷电容,特别是不设计成控制基底处的空间电荷区域,该组件具有在两个横向边界之一处具有相同横向结构的附加层 底座的表面。
    • 93. 发明申请
    • FUEL CELL ELECTRODE-ELECTROLYTE UNIT
    • 电解液单位燃料电池
    • WO1998021777A1
    • 1998-05-22
    • PCT/DE1997002551
    • 1997-11-05
    • FORSCHUNGSZENTRUM JÜLICH GMBHDOHLE, HendrikPEINECKE, VolkerBUSENBENDER, IlonaKELS, Thorsten
    • FORSCHUNGSZENTRUM JÜLICH GMBH
    • H01M08/10
    • H01M8/1009H01M8/0289H01M2008/1095
    • One disadvantage of known fuel cell electrolyte layers is that they do not only let hydrogen ions (protons) through but do the same in part with regard to hydrate sheaths or a part of the fuel. In methanol driven fuel cells the electrolyte enables methanol molecules to pass through. The problem is solved by an electrode-electrolyte unit wherein the electrolyte is divided up into two electrolyte layers (4, 6) with a blocking layer (5) in between. The blocking layer is made from a non-porous or closed pore material which absorbs protons on one side, emits them on the opposite side and is impervious to all other substances. Preferably, the blocking layer (5) is made from a palladium silver alloy. The electrode-electrolyte unit is suitable for fuel cells involving the use of a fuel whose protons can be catalytically separated on the anode, e.g. hydrogen or methanol.
    • 燃料电池的公知的电解质层,不仅氢离子(质子)发生,但也部分氢离子或燃料的一部分的水合外层的缺点。 当甲醇动力的燃料电池,甲醇分子通过电解质。 问题是控制与电极 - 电解质部,其中所述电解质为两个电解质层(4,6)是分离的,之间其中阻挡层(5)的无孔或封闭孔,质子接收在所述一个侧面和相对的侧 质子供不透布置材料的所有其他物质。 阻挡层(5)优选地由钯 - 银合金构成。 用于燃料电极 - 电解质单元适合用于燃料电池中,在阳极处从催化质子被分出,例如 氢或甲醇。
    • 96. 发明申请
    • PIN LAYER SEQUENCE ON A PEROVSKITE
    • PIN-层序列上的钙钛矿
    • WO1997041081A1
    • 1997-11-06
    • PCT/DE1997000822
    • 1997-04-23
    • FORSCHUNGSZENTRUM JÜLICH GMBHSPEIER, WolfgangSZOT, Krzysztof
    • FORSCHUNGSZENTRUM JÜLICH GMBH
    • C04B35/47
    • C04B41/89H01L21/764
    • The invention relates to a process for producing a pin layer sequence which has an AO (ABO3)m layer, a B layer rich in oxides and an ABO3 layer therebetween. It also relates to a layer sequence produced according to the process. In the process AO layers are displaced within a perovskite of the type ABO3 (e.g. SrTiO3, BaTiO3, PbTiO3 or KNbO3) in that said perovskite is subjected to oxidising or reducing conditions at high temperatures. Said displacement results in the desired layer sequence on the surface of the perovskite. In another embodiment, a steady direct current initially flows through the perovskite. The current flowing through the perovskite results in electromigration of the oxygen ions, in particular along two-dimensional defects in the perovskite. Said ions migrate from the cathode towards the anode should two electrodes have been attached to the perovskite to produce the current flow. Electromigration causes the formation of a chemical oxygen concentration gradient in the vicinity of the anode thereby producing additional segregation from AO complexes. Consequently, a pin layer sequence is produced below the anode (the same is true for bombardment with electrons).
    • 本发明涉及一种用于生产具有AO销层序列的方法<>(ABO 3)米,富B氧化物层和居间层ABO 3。 本发明还涉及根据制造的层序列的方法。 一种方法,根据AO层umverlagert ABO 3型(例如,钛酸锶,钛酸钡,钛酸铅或的KNbO 3)的钙钛矿中。 这是通过暴露的氧化或在高温下的还原条件来实现的。 通过Umverlagerung形成钙钛矿的表面上的层的所期望的序列。 第一可替换地流过的钙钛矿,一个恒定的直流电流。 的电流通过钙钛矿的流动导致了氧离子的电迁移,特别是沿着在钙钛矿的二维缺陷。 这些迁移从朝向当两个电极被附加到当前流产生在钙钛矿阳极阴极。 电迁移导致阳极附近的化学氧浓度的形成。 以这种方式,AO的复合物的另外的偏析实现。 下的阳极(当用电子轰击相同)被制造为一个销层序列。
    • 97. 发明申请
    • THREE-COLOUR SENSOR WITH A PIN OR NIP SERIES OF LAYERS
    • 用大头针或NIP层序列中有三个颜色传感器
    • WO1997038450A1
    • 1997-10-16
    • PCT/DE1997000713
    • 1997-04-07
    • FORSCHUNGSZENTRUM JÜLICH GMBHSTIEBIG, HelmutFÖLSCH, JoachimKNIPP, Dietmar
    • FORSCHUNGSZENTRUM JÜLICH GMBH
    • H01L31/105
    • H01L31/1055
    • A structure of several i-layers is limited on one side by a p-layer and on the other side by an n-layer. The structure has means that form said i-layers in such a way that at least in the boundary area between two adjacent i-layers (i , i ), seen in the light incidence direction, the bandgap Eg (I) of the first i-layer (i ) closer to the light input side is larger than the bandgap Eg (II) of the second i-layer (i ) adjacent to the first and further removed from the light input side. In addition, in the boundary area between two adjacent i-layers (i , i ), in the direction from the p-layer to the n-layer, the product mu tau (I) of the i-layer (i ) further removed from the n-layer is larger than the product mu tau (II) of the i-layer (i ) closer to the n-layer. A structure is thus obtained for forming a colour sensor which generates signals which need to be superimposed to a lesser extent for image processing. The structure is preferably designed as a pin- or nip-structure.
    • 本发明涉及一种具有多个i层中的哪一个在一侧由在另一侧的p层由n层界定的结构。 在这种情况下,用于形成所述结构,所述i层,即在光入射方向的至少效果(I I )在光入射侧的相应一个的两个相邻i层中,带隙Eg(I)的边界区域相邻越近的 ,前者i层(I )比带隙Eg更大(II)相邻的与它的,光入射侧较远的,第二i层(i )。 此外,在从对 - 从n层的i型层进一步的n层的方向是在两个相邻的i层的边界区域中的至少(I I )的产物亩的tau(I)( I )比相邻越近的i层,n型层的产品的tau亩(II)的情况下(I )。 以这种方式,用于形成彩色传感器设置结构中,所产生的信号,可能需要用于图像处理的减小叠加。 优选地,形成的结构作为一个销或nip结构。
    • 99. 发明申请
    • MAGNETIC FIELD MEASURING ARRANGEMENT
    • 测量器具,用于测量FIELDS
    • WO1997031273A2
    • 1997-08-28
    • PCT/DE1997000315
    • 1997-02-21
    • FORSCHUNGSZENTRUM JÜLICH GMBHZIMMERMANN, EgonBRANDENBURG, GünterCLEMENS, UweHALLING, Horst
    • FORSCHUNGSZENTRUM JÜLICH GMBH
    • G01R33/035
    • G01R33/0356
    • The invention concerns an arrangement for measuring magnetic fields using a SQUID. To that end, a hybrid regulation system is provided which comprises means for converting a measuring signal (1) from a SQUID (3) into a voltage signal (4) for an analog proportional controller (5), the compensation signal (6) calculated by the proportional controller (5) forming the input signal of a digital integral controller (9, 11, 13). This signal (6) is digitized by an analog-to-digital converter (9) and fed to an arithmetic-logic unit (11) which calculates the compensation signal (12) of the integral controller, and the digital signal (12) is converted by a digital-to-analog converter (13) into an analog signal (14). Finally, an analog summer (15) forms the total compensation signal (16) from the compensation signal (6) of the analog proportional controller (5) and the compensation signal (12) of the digital integral controller (14). The total compensation signal (16) is then converted into a compensation flow (8) via a linear voltage-flow converter (7). The arithmetic-logic unit (11) also controls a resetting unit and a fluxion counter and calculates the output signal (17).
    • 本发明通过一个SQUID的装置涉及一种用于磁场测量的测量装置。 为此,提供了一种混合动力控制,其包括装置,使得测量信号(1)一SQUID(3)转换成电压信号的(4)被转换成模拟的P控制器(5)和(5)计算出的P-控制器 补偿信号(6),则数字I-调节器(9,11,13)的输入信号。 施加到该信号(6),我们通过DA数字化由AD转换器(9)和一个计算单元(11),所述运算单元(11)计算I控制器和所述数字信号(12)的补偿信号(12) 转换器(13)被转换成模拟信号(14)。 最后,由此形成补偿信号的模拟加法元件(15)(6)所述模拟的P控制器(5)和数字I-控制器(14)的总的补偿信号(16)的补偿信号(12),并且这是再一个 线性电压 - 流量转换器(7)被转换成补偿流(8),复位单元和通量量子计数器,以及从所述运算单元(11)的输出信号(17)的计算制成。