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    • 26. 发明授权
    • Synthesizer of an oscillating signal
    • 振荡信号的合成器
    • US08610512B2
    • 2013-12-17
    • US13451913
    • 2012-04-20
    • Jean-Philippe MichelMichaël Quinsat
    • Jean-Philippe MichelMichaël Quinsat
    • H03B5/00
    • H03B15/006H03B15/00
    • A synthesizer includes a second frequency-synthesizing stage comprising a radiofrequency oscillator configured to oscillate at a frequency αfo when it is synchronized with a signal s0(t), where α is a rational number different from one such that αf0=ft. The radiofrequency oscillator has a magnetoresistive device within which there flows a spin-polarized electrical current to generate a signal st(t) oscillating at the frequency ft on an output electrode connected to the rendering terminal. This device is formed by a stack of magnetic and non-magnetic layers, a synchronization terminal for synchronizing the frequency of the oscillating signal st(t) with the frequency of the signal received at the synchronization terminal. The synchronization terminal being connected to the output terminal of the first stage to receive the signal s0(t).
    • 合成器包括第二频率合成级,其包括射频振荡器,其被配置为当与信号s0(t)同步时以alfafo频率振荡,其中α是不同于alphaf0 = ft的有理数。 射频振荡器具有磁阻器件,在该磁阻器件中,流过自旋极化电流以产生在连接到再现终端的输出电极上以频率ft振荡的信号st(t)。 该装置由磁性层和非磁性层的堆叠形成,同步终端用于使振荡信号st(t)的频率与在同步终端处接收的信号的频率同步。 同步终端连接到第一级的输出端以接收信号s0(t)。
    • 29. 发明授权
    • Magnetic field sensing system using spin-torque diode effect
    • 磁场感应系统采用自旋转矩二极管效应
    • US08416539B2
    • 2013-04-09
    • US12188183
    • 2008-08-07
    • Matthew J. CareyJeffrey R. ChildressStefan Maat
    • Matthew J. CareyJeffrey R. ChildressStefan Maat
    • G11B5/33G11B5/127
    • G11B5/3909B82Y10/00B82Y25/00G01R33/098G11B5/3932G11B2005/3996H01F10/3259H01F10/3286H03B15/006
    • A magnetic field sensing system with a current-perpendicular-to-the-plane (CPP) sensor, like that used for giant magnetoresistive (GMR) and tunneling magnetoresistive (TMR) spin-valve (SV) sensors, operates in a mode different from conventional GMR-SV and TMR-SV systems. An alternating-current (AC) source operates at a fixed selected frequency and directs AC perpendicularly through the layers of the CPP sensor, with the AC amplitude being high enough to deliberately induce a spin-torque in the CPP sensor's free layer. The AC-induced spin-torque at the selected frequency causes oscillations in the magnetization of the free layer that give rise to a DC voltage signal VDC. VDC is a direct result of only the oscillations induced in the free layer. The value of VDC will change in response to the magnitude of the external magnetic field being sensed and as the free layer is driven in and out of resonance with the AC.
    • 与用于巨磁阻(GMR)和隧道磁阻(TMR)自旋阀(SV)传感器的电流垂直平面(CPP)传感器的磁场感测系统以不同于 常规GMR-SV和TMR-SV系统。 交流(AC)源以固定的选定频率工作,并直接通过CPP传感器的层引导AC,AC振幅足够高以故意诱导CPP传感器自由层中的自旋扭矩。 所选频率下的交流感应自旋转矩引起自由层的磁化振动,产生直流电压信号VDC。 VDC是仅在自由层中引起的振荡的直接结果。 VDC的值将响应于被感测的外部磁场的大小而变化,并且自由层被驱动进入和退出与AC谐振。