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    • 1. 发明授权
    • Superconductor filter device and manufacturing method thereof
    • 超导体滤波器及其制造方法
    • US06609290B1
    • 2003-08-26
    • US09553330
    • 2000-04-20
    • Kuniharu Takahashi
    • Kuniharu Takahashi
    • H01L3924
    • H01P1/20363H01P1/30Y10S505/854Y10T29/49014
    • A superconductor filter is stored in a hermetic filter case so that electrical connection can be provided between the superconductor filter and the outside of the hermetic filter case. The hermetic filter case is stored in a hermetic outer case so that electrical connection can be provided between the superconductor filter and the outside of the hermetic outer case and so that air/gas flow through pipes can be implemented between the inside of the hermetic filter case and the outside of the hermetic outer case. The hermetic filter case and the hermetic outer case are evacuated into vacuum, and the superconductor filter is cooled below its critical temperature. After the superconducting state of the superconductor filter could be observed, gas that does not deteriorate or react with the superconductor filter is gradually packed in the hermetic filter case and thereby the dielectric constant around the superconductor filter is raised from the dielectric constant of vacuum. The amount of the gas packed in the hermetic filter case is increased/decreased while observing transmission characteristics (center frequency etc.) of the superconductor filter, until desired transmission characteristics are obtained. Thereafter, the hermetic filter case is hermetically sealed so that the amount of the gas in the hermetic filter case will thereafter be fixed.
    • 超导体滤波器存储在密闭的过滤器壳体中,使得可以在超导体滤波器和密封过滤器壳体的外部之间提供电连接。 密封的过滤器壳体存储在密封的外壳中,使得可以在超导体过滤器和密封外壳的外部之间提供电连接,并且可以在密封过滤器壳体的内部之间实现通过管道的空气/气体流动 和密封外壳的外侧。 密封过滤器外壳和密封外壳抽真空,超导体过滤器被冷却到临界温度以下。 在可以观察到超导体滤波器的超导状态之后,不会劣化或与超导体滤波器反应的气体逐渐被封装在密封的过滤器壳体中,从而使超导体滤波器周围的介电常数从真空介电常数提高。 在观察超导体滤波器的传输特性(中心频率等)的同时,包装在密闭式过滤器壳体中的气体的量增加/减小,直到获得所需的传输特性。 此后,密封过滤器壳体被气密地密封,使得密封过滤器壳体中的气体量此后将被固定。
    • 2. 发明授权
    • Two-dimensional, Josephson-array, voltage-tunable, high-frequency
oscillator
    • 二维,约瑟夫逊阵列,电压可调谐,高频振荡器
    • US5114912A
    • 1992-05-19
    • US699282
    • 1991-05-13
    • Samuel P. Benz
    • Samuel P. Benz
    • H01L27/18H03B15/00
    • H03B15/003H01L27/18H03B2200/0022Y10S505/702Y10S505/854
    • A two-dimensional array of Josephson junctions is used as a high-frequency oscillator capable of emitting coherent power of predetermined frequencies since the geometry of the two-dimensional array allows the individual Josephson junctions to phase lock at predetermined frequencies. The array is controlled at a given voltage and excited by the application of DC current through the array, in effect providing a rapidly tunable DC-to-AC converter at GHz and THz frequencies. The oscillator operates without the application of external high frequency signals or a connection to a cavity resonator. Load matching and other adjustments can be made by selecting the appropriate number of Josephson junctions in the array, selecting a damping factor which determines non-hysteretic operation, adding resistive shunts or a superconducting ground plane. The two-dimensional array used as an oscillator has advantages over one dimensional arrays in that voltage equalization from junction-to-junction occurs naturally so that phase locking is less likely to be affected by non-identical junctions, greater power output can be realized, an output having a narrower line width is produced and impedance matching is relatively easy.
    • 使用约瑟夫逊结的二维阵列作为能够发射预定频率的相干功率的高频振荡器,因为二维阵列的几何形状允许各个约瑟夫逊结以预定频率锁相。 该阵列被控制在给定的电压并且通过施加直流电流通过阵列而被激励,实际上提供了在GHz和THz频率下的快速可调DC-AC转换器。 振荡器在不施加外部高频信号或连接到空腔谐振器的情况下工作。 可以通过选择阵列中适当数量的约瑟夫逊结,选择确定非迟滞操作的阻尼因子,添加电阻分流器或超导接地平面来进行负载匹配和其他调整。 用作振荡器的二维阵列具有超过一维阵列的优点,因为从结到结的电压均衡自然发生,使得相位锁定不太可能受到不相同的结的影响,可以实现更大的功率输出, 产生具有较窄线宽的输出,并且阻抗匹配相对容易。
    • 4. 发明授权
    • Multimode oscillators
    • US3916340A
    • 1975-10-28
    • US47766474
    • 1974-06-10
    • WISCONSIN ALUMNI RES FOUND
    • SCOTT ALWYN C
    • H01J29/36H01L39/00H03B15/00H03B7/06
    • H01J29/36H01L39/00H03B15/00Y10S505/854
    • A multimode oscillator is disclosed, comprising an array of interconnected oscillator elements distributed over at least two dimensions. The oscillator elements include a grid or network of impedance elements. Three or more inductive (capacitive) elements may radiate from each junction point in the grid, and a capacitive (inductive) element may be shunted to ground from each junction point. Other arrangements of impedance elements are also possible. The multimode oscillator may be either passive or active. In a passive oscillator, the oscillations are not sustained but rather are damped by the resistance elements and other losses in the oscillator. A passive oscillator may be excited into various simultaneous modes of oscillation by coupling the output of a white noise generator, or some other white signal source, to the multimode oscillator. The resulting oscillations are picked up and analyzed as to their frequency components. A bank of filters may be employed to separate the various frequency components. Digital logic circuits may be employed to analyze the signals from the filters. Sustained oscillations may be produced in a passive multimode oscillator by providing feedback means between the output and input of the oscillator. Such feedback means may include an amplifier and a nonlinear inductive element or some other nonlinear element which makes it possible to sustain a number of different modes of oscillation simultaneously. An active multimode oscillator employs active elements capable of sustaining the oscillations in the oscillator. Such active elements may include various negative resistance elements such as tunnel diodes. The multimode oscillator may utilize superconductive elements which may be arranged to form a superconductive grid or network to provide an array of inductive elements. The capacitive elements may be provided by the distributed capacitance between the superconductive grid and a superconductive ground plate or surface. The superconductive multimode oscillator may be either passive or active. Active elements may be provided by superconductive tunneling through thin barrier elements between portions of the superconductive grid and the ground plate. The active tunnel elements may also be radiation sensitive.
    • 8. 发明授权
    • Sns supercurrent device
    • SNS超流量器件
    • US3751721A
    • 1973-08-07
    • US3751721D
    • 1971-12-22
    • BELL TELEPHONE LABOR INC
    • FULTON T
    • H01L39/06H01L39/22H01L
    • H01L39/22Y10S505/854
    • An improved SNS supercurrent device comprises a pair of superconductive regions, a relatively thick insulative region contiguous with and separating the superconductive regions from one another, and a normal metal region contiguous with both superconductive regions. The insulative region is of sufficient thickness to prevent substantial supercurrent tunneling therethrough when a current source is connected between the superconductive regions. Consequently, current, following the path of least resistance, flows in a path including the normal metal region. The junction defined by the normal metal region has a significantly reduced cross-sectional area which in turn means the device has lower critical supercurrents and higher resistances than heretofore attainable in SNS structures.
    • 一种改进的SNS超电流装置包括一对超导区域,与超导区域彼此相邻并且分离超导区域的相对较厚的绝缘区域和与两个超导区域相邻的正常金属区域。 当电流源连接在超导区域之间时,绝缘区域具有足够的厚度以防止实质上的超级电流穿透。 因此,在最小电阻的路径之后的电流在包括正常金属区域的路径中流动。 由正常金属区域限定的接头具有明显减小的横截面面积,这又意味着该装置具有比迄今为止可在SNS结构中获得的更低的临界超电流和更高的电阻。
    • 10. 发明授权
    • Fluxon oscillators utilizing a ring shaped Josephson junction
    • 利用环形约瑟夫逊结的Fluxon振荡器
    • US4181902A
    • 1980-01-01
    • US923955
    • 1978-07-12
    • Alwyn C. Scott
    • Alwyn C. Scott
    • H01L39/22H03B15/00
    • H01L39/223Y10S505/854
    • The fluxon oscillators for producing electromagnetic radiation having a wavelength shorter than the shortest radio waves, but longer than the longest infrared radiation, may comprise two closely spaced superconductive ring-shaped members having a ring-shaped Josephson junction barrier therebetween capable of supporting the tunnelling of superconductive electrons across such barrier, a source of magnetic flux for initially producing at least one fluxon in the barrier, a power supply for producing an electrical biasing current between the superconductive members and across the barrier for causing movement of the fluxon along and around the ring-shaped barrier in a closed path, and a plurality of centers to produce enhanced superconductive electron current across the barrier, such centers being spaced around the ring-shaped barrier for causing cyclical variations in the velocity of the fluxon and thereby causing the radiation of electromagnetic energy at a frequency corresponding to the frequency of such cyclical variations. Such centers may comprise localized microshorts or weak links which are conductive to normal tunnelling electrons and exhibit enhanced tunnelling by superconductive electrons. Such weak links may be made of a normally conductive metal, such as copper, silver or gold. The superconductive members may be in the form of superimposed ring-shaped layers with the barrier sandwiched therebetween, or in the form of concentric inner and outer ring-shaped layers, with the barrier being disposed between the edges thereof. Such centers may also be provided by photoconductive material in the barrier, illuminated by a pattern of illumination.
    • 用于产生具有比最短无线电波长但长于最长的红外辐射的波长的电磁辐射的磁通振荡器可以包括两个紧密间隔的超导环形构件,它们之间具有环形约瑟夫逊结屏障,能够支撑隧道 跨越这种势垒的超导电子,用于最初在阻挡层中产生至少一个通量的磁通源,用于在超导构件之间产生电偏置电流并且跨越阻挡层的电源,用于引起磁通管沿着和环绕环的运动 形状的屏障,以及多个中心,以产生穿过屏障的增强的超导电子电流,这些中心围绕环形屏障间隔开,以引起磁通量的速度的周期性变化,从而导致电磁辐射 能量以对应于f的频率 这种周期性变化的需求。 这样的中心可以包括对正常隧道电子导电并且通过超导电子表现出增强的隧道效应的局部微连线或弱连接。 这种弱连接可以由常规导电的金属制成,例如铜,银或金。 超导构件可以是叠置的环形层的形式,其中屏障夹在其间,或以同心的内圈和外环形层的形式,其中屏障设置在其边缘之间。 这样的中心也可以由屏障中的光导材料提供,由照明模式照亮。