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    • 1. 发明授权
    • Computations using a polychronous wave propagation system
    • 使用同步波传播系统的计算
    • US09110771B2
    • 2015-08-18
    • US13015147
    • 2011-01-27
    • Frank C. HoppensteadtVarun NarendraEugene M. Izhikevich
    • Frank C. HoppensteadtVarun NarendraEugene M. Izhikevich
    • H04Q5/22G06F15/00G06N99/00
    • G06K7/10366G06F15/00G06F17/11G06N3/049G06N99/00
    • The present invention relates to a polychronous wave propagation system that is based on relative timing between two or more propagated waves through a wave propagation medium. The relative timing may be associated with interference patterns of energy between the propagated waves. Operational behavior of the polychronous wave propagation system is based on the relative timing of the propagated waves and distances between initiators that transmit the propagated waves and responders that receive the propagated waves. The operational behavior may include arithmetical computations, memory storage, Boolean functions, frequency-based computations, or the like. The polychronous wave propagation system relies on time delays between the propagated waves that result from propagation velocities of the propagated waves through the wave propagation medium. By incorporating the time delays into the system, operational capacity may be greatly enhanced.
    • 本发明涉及一种基于通过波传播介质的两个或更多个传播波之间的相对定时的同步波传播系统。 相对定时可以与传播波之间的能量的干涉图案相关联。 同步波传播系统的操作行为是基于传播波的相对定时和发射传播波的发射器和接收传播波的响应器之间的距离。 操作行为可以包括算术计算,存储器存储,布尔函数,基于频率的计算等。 同步波传播系统依赖于通过波传播介质传播的波的传播速度所产生的传播波之间的时间延迟。 通过将时间延迟并入系统,可以大大提高运行能力。
    • 2. 发明授权
    • Phase-locked loop oscillatory neurocomputer
    • 锁相环振荡神经计算机
    • US07280989B1
    • 2007-10-09
    • US09771019
    • 2001-01-26
    • Frank C. HoppensteadtEugene M. Izhikevich
    • Frank C. HoppensteadtEugene M. Izhikevich
    • G06E1/00G06E3/00G06F15/18G06G7/00G06N3/00
    • G06N3/049G06K9/46
    • A neural network computer (20) includes a weighting network (21) coupled to a plurality of phase-locked loop circuits (251-25N). The weighting network (21) has a plurality of weighting circuits (C11, . . . , CNN) having output terminals connected to a plurality of adder circuits (311-31N). A single weighting element (Ckj) typically has a plurality of output terminals coupled to a corresponding adder circuit (31k). Each adder circuit (31k) is coupled to a corresponding bandpass filter circuit (31k) which is in turn coupled to a corresponding phase-locked loop circuit (25k). The weighting elements (C1,1, . . . , CN,N) are programmed with connection strengths, wherein the connection strengths have phase-encoded weights. The phase relationships are used to recognize an incoming pattern.
    • 神经网络计算机(20)包括耦合到多个锁相环电路(25-125N)的加权网络(21)。 加权网络(21)具有多个具有连接到多个加法器电路(31')的输出端的加权电路(C 11,...,C N N N) SUB> 1< N< N< N>)。 单个加权元件(C j j>))。。。。。。。。。。。。。。。。。。。。。。。。。。。。。。。。 每个加法器电路(31KK)耦合到对应的带通滤波器电路(31K),该相应的带通滤波器电路又耦合到相应的锁相环电路(25 k )。 加权元件(C 1,1,...,C N,N N)用连接强度编程,其中连接强度具有相位编码权重。 相位关系用于识别输入模式。
    • 3. 发明申请
    • COMPUTATIONS USING A POLYCHRONOUS WAVE PROPAGATION SYSTEM
    • 使用聚合波传播系统的计算
    • US20140025716A1
    • 2014-01-23
    • US13015147
    • 2011-01-27
    • Frank C. HoppensteadtVarun Narendra
    • Frank C. HoppensteadtVarun Narendra
    • G06F15/00
    • G06K7/10366G06F15/00G06F17/11G06N3/049G06N99/00
    • The present invention relates to a polychronous wave propagation system that is based on relative timing between two or more propagated waves through a wave propagation medium. The relative timing may be associated with interference patterns of energy between the propagated waves. Operational behavior of the polychronous wave propagation system is based on the relative timing of the propagated waves and distances between initiators that transmit the propagated waves and responders that receive the propagated waves. The operational behavior may include arithmetical computations, memory storage, Boolean functions, frequency-based computations, or the like. The polychronous wave propagation system relies on time delays between the propagated waves that result from propagation velocities of the propagated waves through the wave propagation medium. By incorporating the time delays into the system, operational capacity may be greatly enhanced.
    • 本发明涉及一种基于通过波传播介质的两个或更多个传播波之间的相对定时的同步波传播系统。 相对定时可以与传播波之间的能量的干涉图案相关联。 同步波传播系统的操作行为是基于传播波的相对定时和发射传播波的发射器和接收传播波的响应器之间的距离。 操作行为可以包括算术计算,存储器存储,布尔函数,基于频率的计算等。 同步波传播系统依赖于通过波传播介质传播的波的传播速度所产生的传播波之间的时间延迟。 通过将时间延迟并入系统,可以大大提高运行能力。
    • 4. 发明授权
    • Controllable oscillator blocks
    • 可控振荡器模块
    • US07783584B1
    • 2010-08-24
    • US11866613
    • 2007-10-03
    • Frank C. Hoppensteadt
    • Frank C. Hoppensteadt
    • G06E1/00G06E3/00G06F15/18G06G7/00G06N3/02
    • G06N3/049G06N3/0635
    • The present invention mimics certain behaviors of a human brain using at least one frequency controllable oscillator block that has multiple operating frequency regions, such that some of the regions tend to lock on to a frequency, while other regions do not have any locking tendencies. A stimulation using at least one stimulation signal based on information input to the system may alter the regions and determine a stable final frequency after a brief processing interval. A control system may process the final frequency to provide system information. A controllable oscillator block may have at least one basin of attraction that corresponds with a stable region of the stimulation signal. Additionally, the controllable oscillator block may function outside of a basin of attraction that corresponds with a non-stable region of the stimulation signal.
    • 本发明使用具有多个工作频率区域的至少一个频率可控振荡器模块来模拟人类大脑的某些行为,使得一些区域倾向于锁定到频率,而其他区域不具有任何锁定倾向。 基于输入到系统的信息使用至少一个刺激信号的刺激可以改变区域并且在短暂的处理间隔之后确定稳定的最终频率。 控制系统可以处理最终频率以提供系统信息。 可控振荡器块可以具有与刺激信号的稳定区域对应的至少一个吸引盆。 此外,可控振荡器块可以在对应于刺激信号的非稳定区域的吸引盆地之外起作用。
    • 5. 发明授权
    • Oscillatary neurocomputers with dynamic connectivity
    • 具有动态连接性的振荡神经计算机
    • US06957204B1
    • 2005-10-18
    • US09831812
    • 1999-11-12
    • Frank C. HoppensteadtEugene Izhikevich
    • Frank C. HoppensteadtEugene Izhikevich
    • G06F15/18G06N3/04G06N3/063
    • G06N3/049G06N3/0635
    • A neurocomputer (50) comprises n oscillating processing elements (60A, 60B, 60C, 60D and 60E) that communicate through a common medium (70) so that there are required only n connective junctions (80A, 80B, 80C, 80D and 80E). A rhythmic external forcing input (90) modulates the oscillatory frequency of the medium (70) which, in turn, is imparted to the n oscillators (60A, 60B, 60C, 60D and 60E). Any two oscillators oscillating at different frequencies may communicate provided that input's power spectrum includes the frequency equal to the difference between the frequencies of the two oscillators in question. Thus, selective communication, or dynamic connectivity, between different neurocomputer oscillators occurs due to the frequency modulation of the medium (70) by external forcing.
    • 神经计算机(50)包括通过公共介质(70)通信的n个振荡处理元件(60A,60B,60C,60D和60E),使得仅需要n个连接结(80A,80B ,80℃,80℃和80℃)。 节奏外部强制输入(90)调制介质(70)的振荡频率,其又被赋予n个振荡器(60A,60B,60C,60D和60E)。 任何以不同频率振荡的两个振荡器可以通信,只要输入的功率谱包括等于所讨论的两个振荡器的频率之间的差的频率。 因此,由于外部强制的介质(70)的频率调制,发生不同神经计算机振荡器之间的选择性通信或动态连接。
    • 6. 发明申请
    • AGGREGATED SPIN-TORQUE NANO-OSCILLATORS
    • 聚集的旋转扭矩纳米振荡器
    • US20120062220A1
    • 2012-03-15
    • US13187724
    • 2011-07-21
    • Frank C. HoppensteadtAndrew D. KentFerran Macià Bros
    • Frank C. HoppensteadtAndrew D. KentFerran Macià Bros
    • G01R33/02H03B9/10
    • G01R33/1284B82Y25/00G01R33/06G01R33/093G01R33/36H03B9/10H03B15/006
    • A nano-oscillator magnetic wave propagation system has a group of aggregated spin-torque nano-oscillators (ASTNOs), which share a magnetic propagation material. Each of the group of ASTNOs is disposed about an emanating point in the magnetic propagation material. During a non-wave propagation state of the nano-oscillator magnetic wave propagation system, the magnetic propagation material receives a polarizing magnetic field. During a wave propagation state of the nano-oscillator magnetic wave propagation system, each of the group of ASTNOs initiates spin waves through the magnetic propagation material, such that a portion of the spin waves initiated from each of the group of ASTNOs combine to produce an aggregation of spin waves emanating from the emanating point. The aggregation of spin waves may provide a sharper wave front than wave fronts of the individual spin waves initiated from each of the group of ASTNOs.
    • 纳米振荡器磁波传播系统具有共享磁传播材料的一组聚集的自旋扭矩纳秒振荡器(ASTNO)。 ASTNO组中的每一个都围绕磁传播材料中的一个发射点设置。 在纳米振荡器磁波传播系统的非波传播状态下,磁传播材料接收偏振磁场。 在纳米振荡器磁波传播系统的波传播状态期间,所述一组ASTNO中的每一个通过磁传播材料引发自旋波,使得从所述一组ASTNO中的每一个引发的一部分自旋波组合以产生 从辐射点发出的自旋波的聚集。 自旋波的聚集可以提供比从ASTNO组中的每一个发起的单个旋转波的波前更尖锐的波前。
    • 7. 发明授权
    • Aggregated spin-torque nano-oscillators
    • 聚合自旋扭矩纳米振荡器
    • US08629729B2
    • 2014-01-14
    • US13187724
    • 2011-07-21
    • Frank C. HoppensteadtAndrew D. KentFerran Macià Bros
    • Frank C. HoppensteadtAndrew D. KentFerran Macià Bros
    • H03L7/26
    • G01R33/1284B82Y25/00G01R33/06G01R33/093G01R33/36H03B9/10H03B15/006
    • A nano-oscillator magnetic wave propagation system has a group of aggregated spin-torque nano-oscillators (ASTNOs), which share a magnetic propagation material. Each of the group of ASTNOs is disposed about an emanating point in the magnetic propagation material. During a non-wave propagation state of the nano-oscillator magnetic wave propagation system, the magnetic propagation material receives a polarizing magnetic field. During a wave propagation state of the nano-oscillator magnetic wave propagation system, each of the group of ASTNOs initiates spin waves through the magnetic propagation material, such that a portion of the spin waves initiated from each of the group of ASTNOs combine to produce an aggregation of spin waves emanating from the emanating point. The aggregation of spin waves may provide a sharper wave front than wave fronts of the individual spin waves initiated from each of the group of ASTNOs.
    • 纳米振荡器磁波传播系统具有共享磁传播材料的一组聚集的自旋扭矩纳秒振荡器(ASTNO)。 ASTNO组中的每一个都围绕磁传播材料中的一个发射点设置。 在纳米振荡器磁波传播系统的非波传播状态下,磁传播材料接收偏振磁场。 在纳米振荡器磁波传播系统的波传播状态期间,所述一组ASTNO中的每一个通过磁传播材料引发自旋波,使得从所述一组ASTNO中的每一个引发的一部分自旋波组合以产生 从辐射点发出的自旋波的聚集。 自旋波的聚集可以提供比从ASTNO组中的每一个发起的单个旋转波的波前更尖锐的波前。