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    • 2. 发明申请
    • TEMPERATURE COMPENSATION FOR MEMS DEVICES
    • MEMS器件温度补偿
    • US20140361661A1
    • 2014-12-11
    • US14029927
    • 2013-09-18
    • Silicon Laboratories Inc.
    • Emmanuel P. QuevyDaniel N. Koury, JR.
    • H02N1/00
    • H02N1/00B81B3/0081H03B5/30H03H3/013H03H9/02259H03H2007/006H03H2009/02291H03H2009/02385H03H2009/0248H03H2009/2442H03L1/02H03L1/04Y10T29/49005Y10T29/49117
    • A microelectromechanical system (MEMS) device includes a temperature compensating structure including a first beam suspended from a substrate and a second beam suspended from the substrate. The first beam is formed from a first material having a first Young's modulus temperature coefficient. The second beam is formed from a second material having a second Young's modulus temperature coefficient. The body may include a routing spring suspended from the substrate. The routing spring may be coupled to the first beam and the second beam. The routing spring may be formed from the second material. The first beam and the second beam may have lower spring compliance than the routing spring. The MEMS device may be a resonator and the temperature compensating structure may have dimensions and a location such that the temperature compensation structure modifies a temperature coefficient of frequency of the resonator independent of a mode shape of the resonator.
    • 微机电系统(MEMS)装置包括温度补偿结构,其包括从衬底悬挂的第一光束和从衬底悬挂的第二光束。 第一梁由具有第一杨氏模量温度系数的第一材料形成。 第二梁由具有第二杨氏模量温度系数的第二材料形成。 主体可以包括从基板悬挂的布线弹簧。 路由弹簧可以耦合到第一波束和第二波束。 路由弹簧可以由第二材料形成。 第一光束和第二光束可能具有比布线弹簧更低的弹性柔顺度。 MEMS器件可以是谐振器,并且温度补偿结构可以具有尺寸和位置,使得温度补偿结构独立于谐振器的模式形状来修改谐振器的频率的温度系数。
    • 4. 发明申请
    • METHOD OF TUNING BAW RESONATORS
    • 调谐BAW谐振器的方法
    • US20020158716A1
    • 2002-10-31
    • US09845089
    • 2001-04-27
    • Nokia Mobile Phones Ltd.
    • Tuomas Pensala
    • H01L041/08
    • H03H3/013
    • A method of tuning a bulk acoustic wave device having a piezoelectric layer formed between a top electrode and a bottom electrode, wherein the top electrode has a frame-like structure at an edge portion for reducing spurious resonance in the electrical response of the device. The frame-like structure surrounds a center zone of the top electrode. In order to down-shift the resonance frequency of the device, a tuning layer is provided on the top electrode. In particular, the tuning layer is designed such that it covers at least the entire center zone in order to reduce the spurious resonance introduced by the tuning layer itself. Preferably, the tuning layer covers the center zone as well as the frame-like structure to further reduce the spurious resonance.
    • 一种调谐具有形成在顶部电极和底部电极之间的压电层的体声波器件的方法,其中顶部电极在边缘部分具有框架结构,用于减少器件的电响应中的寄生谐振。 框架状结构围绕顶部电极的中心区域。 为了降低器件的谐振频率,在顶部电极上设置调谐层。 特别地,调谐层被设计成使得其至少覆盖整个中心区域,以便减少由调谐层本身引入的寄生谐振。 优选地,调谐层覆盖中心区域和框架状结构,以进一步减少杂散共振。
    • 5. 发明申请
    • Micromechanical resonator device
    • 微机械谐振器装置
    • US20020069701A1
    • 2002-06-13
    • US09938412
    • 2001-08-23
    • Wan-Thai HsuClark T.-C. Nguyen
    • H03H009/24G01P015/125
    • H03H9/505H03H3/0072H03H3/013H03H9/02362H03H9/02448H03H9/2436H03H9/462H03H2009/02496
    • A micromechanical resonator device is disclosed that utilizes competition between the thermal dependencies of geometrically tailored stresses and Young's modulus to (1) reduce the temperature coefficient (TCf) of the resonance frequencies of the micromechanical resonator device without any additional power consumption; and (2) introduce a zero TCf temperature at which subsequent oven-controlled resonators may be biased. A key feature in this resonator design involves the strategic sizing of the geometries of the resonator and its support structure to harness thermal expansion temperature coefficients that oppose and cancel those of Young's modulus variation. This transforms the original monotonically decreasing resonance frequency versus temperature curve to an S-shaped curve (or a linear one with a much smaller slope), with a smaller overall frequency excursion over a given temperature range, and with points at which the resonance frequency TCf is zero. This design strategy is a key to attaining the needed temperature stability for reference oscillator applications in portable wireless communications and for RF channel-select filter banks. In addition, for cases where the thermal response of a resonator need not be nulled, but rather must satisfy a given shape, this technique can also be used to tailor a specific resonance frequency versus temperature curve.
    • 公开了一种微机械谐振器装置,利用几何量化应力和杨氏模量的热依赖性之间的竞争,(1)降低微机械谐振器装置的谐振频率的温度系数(TCf),而不需要任何额外的功率消耗; 和(2)引入零TCf温度,随后的控温谐振器可能被偏置。 该共振器设计中的一个关键特征涉及谐振器及其支撑结构的几何形状的策略尺寸,以利用对抗和消除杨氏模量变化的热膨胀温度系数。 这将原始单调降低的共振频率对温度曲线转换为S形曲线(或具有小得多的斜率的线性曲线),在给定温度范围内具有较小的总频率偏移,以及谐振频率TCf 是零。 该设计策略是实现便携式无线通信和RF通道选择滤波器组中参考振荡器应用所需的温度稳定性的关键。 此外,对于谐振器的热响应不需要为零而是必须满足给定形状的情况,该技术也可用于定制特定谐振频率对温度曲线。
    • 6. 发明授权
    • Permanent magnet twister
    • 永磁扭矩机
    • US5945899A
    • 1999-08-31
    • US920237
    • 1997-08-25
    • Herbert A. Leupold
    • Herbert A. Leupold
    • G01R23/10H01F7/02H01P1/20H03H3/013H03H7/12H03H11/04H05H7/04H01F7/00
    • H01F7/0278H03H11/04H03H3/013H03H7/12H05H7/04
    • A permanent magnet rectangular bar shaped to form a helix having a centralore and a longitudinal axis. The magnetic orientation of the helical permanent magnet bar is along the longitudinal axis forming a transverse helical magnetic field. An electron beam or charged particle passing near the longitudinal axis experiences acceleration causing the charged particles to radiate creating a high energy radiation source. In another embodiment, first and second permanent magnet helical bars are intertwined together, forming a cylindrical tube, with each of the intertwined helical bars having a magnetic orientation along the longitudinal axis in opposing directions. In another embodiment of the present invention, an iron ribbon or other high permeability magnetic material is interposed between cut-out portions between first and second intertwined helical permanent magnet bars. This effectively augments the transverse magnetic field. A relatively compact permanent magnetic structure that is relatively simple having a desired transverse helical magnetic field is made possible for such applications as free electron lasers or millimeter/microwave radar devices.
    • 永久磁铁矩形条,形状形成具有中心孔和纵向轴线的螺旋。 螺旋形永久磁铁棒的磁性取向沿纵向轴线形成横向螺旋磁场。 通过靠近纵向轴线的电子束或带电粒子经受加速,导致带电粒子辐射,产生高能辐射源。 在另一个实施例中,第一和第二永磁螺旋杆相互缠绕在一起,形成圆柱形管,其中每个相互缠绕的螺旋杆在沿相反方向的纵向轴线上具有磁性取向。 在本发明的另一个实施例中,铁带或其它高磁导率磁性材料介于第一和第二交织的螺旋永久磁铁棒之间的切口部分之间。 这有效地增强了横向磁场。 对于诸如自由电子激光器或毫米/微波雷达装置的应用,使具有所需横向螺旋磁场的相对简单的相对紧凑的永磁结构成为可能。