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    • 2. 发明申请
    • THREE DIMENSIONAL RADIATION DETECTOR
    • 三维辐射探测器
    • US20070040126A1
    • 2007-02-22
    • US11430755
    • 2006-05-09
    • Uri El-HananyArie ShaharShimon KlierAlex TsigelmanEldan Halberthal
    • Uri El-HananyArie ShaharShimon KlierAlex TsigelmanEldan Halberthal
    • G01T1/24G01T1/29H01L27/146H01L25/00
    • G01T1/202G01T1/2018
    • A pixelated detector assembly comprising a stack of thin detector crystals, each detector crystal having a pair of planar surfaces bound by edges substantially thinner than the dimensions of the surfaces. The stack is disposed such that the radiation to be detected is incident on one set of edges of the stack of detector crystals. The dimension of the planar surfaces in the general direction of incidence of the radiation incidence is sufficient to ensure that substantially all of the high energy photons to be detected are absorbed within the depth of the detector assembly. Each of the detector crystals has a two-dimensional pixelated anode array formed on one of its planar surfaces. A cathode is formed on its opposite planar surface, preferably covering substantially all of the surface. The position of interaction of a photon in the plane perpendicular to the direction of the incident radiation, is determined by which of the detector crystals in the stack detects the absorption, and by which of the rows of pixelated anodes in that crystal detects the absorption. The depth of interaction of a photon is determined by the location of the particular anode pixel in the above-mentioned row of pixelated anodes where the photon absorption is detected. The detector assembly is thus able to detect the point of interaction of a photon in all three dimensions.
    • 一种像素化检测器组件,包括薄的检测器晶体的堆叠,每个检测器晶体具有由比表面的尺寸更薄的边缘约束的一对平面。 堆叠被布置成使得待检测的辐射入射在检测器晶体堆叠的一组边缘上。 平面表面在辐射入射的大致入射方向上的尺寸足以确保被检测的基本上所有的高能量光子在检测器组件的深度内被吸收。 每个检测器晶体具有形成在其一个平面表面上的二维像素化阳极阵列。 阴极形成在其相对的平坦表面上,优选覆盖基本上所有的表面。 垂直于入射辐射方向的平面中的光子相互作用的位置由叠层中的哪一个检测器晶体检测到吸收以及该晶体中哪一行的像素化阳极中的哪一行检测到吸收来确定。 光子的相互作用深度由上述行检测到光子吸收的像素化阳极中的特定阳极像素的位置决定。 因此,检测器组件能够检测所有三维中光子的相互作用点。
    • 3. 发明授权
    • Semiconductor gamma-ray detector
    • 半导体伽马射线探测器
    • US06285029B1
    • 2001-09-04
    • US09123754
    • 1998-07-27
    • Arie ShaharUri El-HananyAlex TsigelmanShimon KlierEldan Halberthal
    • Arie ShaharUri El-HananyAlex TsigelmanShimon KlierEldan Halberthal
    • G01T124
    • G01T1/2985G01T1/202G01T1/242G01T1/243G01T1/249
    • A novel semiconductor detector device, consisting of several layers of two dimensional detector modules each module being divided into an array of separate detector cells by means of the pixelation of the electrodes on the surfaces of the modules. The superimposed detector cells in equivalent positions in each layer are in electrical contact with those in the two immediately adjacent layers, such that the whole device effectively becomes a two dimensional array of stacks of individual detector cells, with a common bottom electrode. Current in each detector cell stack, induced by the absorption of a high energy photon in that stack, is measured by means of an integrating charge sensitive amplifier attached to each anode at the top of each cell stack. A large area gamma-ray detector, sufficiently thick to absorb the high energy photons arising from electron-positron annihilation events, is thus obtained, but without the expense associated with the production of a single detector crystal of the required thickness.
    • 一种新颖的半导体检测器装置,由几层二维检测器模块组成,每个模块通过模块表面上的电极的像素化被分成独立的检测器单元的阵列。 每个层中等效位置的叠加的检测器单元与两个紧邻的层中的叠层检测器单元电接触,使得整个器件有效地成为具有公共底部电极的各个检测器单元的堆叠的二维阵列。 通过在每个电池堆顶部连接到每个阳极的积分电荷敏感放大器来测量每个检测器电池堆中由该堆叠中的高能量光子的吸收而引起的电流。 因此,获得了足够厚以吸收由电子 - 正电子湮灭事件引起的高能量光子的大面积γ射线检测器,但没有与所需厚度的单个检测器晶体的生产相关的费用。
    • 4. 发明授权
    • Three dimensional radiation detector
    • 三维辐射探测器
    • US07208740B2
    • 2007-04-24
    • US11430755
    • 2006-05-09
    • Uri El-HananyArie ShaharShimon KlierAlex TsigelmanEldan Halberthal
    • Uri El-HananyArie ShaharShimon KlierAlex TsigelmanEldan Halberthal
    • G01T1/24
    • G01T1/202G01T1/2018
    • A pixelated detector assembly comprising a stack of thin detector crystals, each detector crystal having a pair of planar surfaces bound by edges substantially thinner than the dimensions of the surfaces. The stack is disposed such that the radiation to be detected is incident on one set of edges of the stack of detector crystals. The dimension of the planar surfaces in the general direction of incidence of the radiation incidence is sufficient to ensure that substantially all of the high energy photons to be detected are absorbed within the depth of the detector assembly. Each of the detector crystals has a two-dimensional pixelated anode array formed on one of its planar surfaces. A cathode is formed on its opposite planar surface, preferably covering substantially all of the surface. The position of interaction of a photon in the plane perpendicular to the direction of the incident radiation, is determined by which of the detector crystals in the stack detects the absorption, and by which of the rows of pixelated anodes in that crystal detects the absorption. The depth of interaction of a photon is determined by the location of the particular anode pixel in the above-mentioned row of pixelated anodes where the photon absorption is detected. The detector assembly is thus able to detect the point of interaction of a photon in all three dimensions.
    • 一种像素化检测器组件,包括薄的检测器晶体的堆叠,每个检测器晶体具有由比表面的尺寸更薄的边缘约束的一对平面。 堆叠被布置成使得待检测的辐射入射在检测器晶体堆叠的一组边缘上。 平面表面在辐射入射的大致入射方向上的尺寸足以确保被检测的基本上所有的高能量光子在检测器组件的深度内被吸收。 每个检测器晶体具有形成在其一个平面表面上的二维像素化阳极阵列。 阴极形成在其相对的平坦表面上,优选覆盖基本上所有的表面。 垂直于入射辐射方向的平面中的光子相互作用的位置由叠层中的哪一个检测器晶体检测到吸收以及该晶体中哪一行的像素化阳极中的哪一行检测到吸收来确定。 光子的相互作用深度由上述行检测到光子吸收的像素化阳极中的特定阳极像素的位置决定。 因此,检测器组件能够检测所有三维中光子的相互作用点。
    • 5. 发明授权
    • Three dimensional radiation detector
    • US07166848B2
    • 2007-01-23
    • US10179909
    • 2002-06-25
    • Uri El-HananyArie ShaharShimon KlierAlex TsigelmanEldan Halberthal
    • Uri El-HananyArie ShaharShimon KlierAlex TsigelmanEldan Halberthal
    • G01T1/24
    • G01T1/202G01T1/2018
    • A pixelated detector assembly comprising a stack of thin detector crystals, each detector crystal having a pair of planar surfaces bound by edges substantially thinner than the dimensions of the surfaces. The stack is disposed such that the radiation to be detected is incident on one set of edges of the stack of detector crystals. The dimension of the planar surfaces in the general direction of incidence of the radiation incidence is sufficient to ensure that substantially all of the high energy photons to be detected are absorbed within the depth of the detector assembly. Each of the detector crystals has a two-dimensional pixelated anode array formed on one of its planar surfaces. A cathode is formed on its opposite planar surface, preferably covering substantially all of the surface. The position of interaction of a photon in the plane perpendicular to the direction of the incident radiation, is determined by which of the detector crystals in the stack detects the absorption, and by which of the rows of pixelated anodes in that crystal detects the absorption. The depth of interaction of a photon is determined by the location of the particular anode pixel in the above-mentioned row of pixelated anodes where the photon absorption is detected. The detector assembly is thus able to detect the point of interaction of a photon in all three dimensions.
    • 6. 发明授权
    • Gamma-ray detector for coincidence detection
    • 伽马射线探测器用于重合检测
    • US06765213B2
    • 2004-07-20
    • US09918371
    • 2001-07-30
    • Arie ShaharUri El-HananyAlex TsigelmanShimon KlierEldan Halberthal
    • Arie ShaharUri El-HananyAlex TsigelmanShimon KlierEldan Halberthal
    • G01T124
    • G01T1/2928
    • A semiconductor coincidence detector device including at least a first and a second detector crystal array, each having a first and second surface, an array of pixellated anodes formed on each of the first surfaces, an array of segmented cathodes formed on each of the second surfaces, essentially each of the pixellated anodes being connected to an anode electronic channel for generating a first electrical signal corresponding to the energy of a photon impinging in the semiconductor, and essentially each of the segmented cathodes being connected to a cathode electronic channel for generating an electrical coincidence trigger signal on detection of a photon impinging in the semiconductor, the first electrical signal being read only from anodes located opposite the cathode segment generating the trigger signal.
    • 一种半导体符合检测器件,至少包括第一和第二检测器晶体阵列,每个具有第一和第二表面,形成在每个第一表面上的像素化​​阳极阵列,形成在每个第二表面上的分段阴极阵列 ,基本上每个像素化阳极连接到阳极电子通道,用于产生对应于入射在半导体中的光子的能量的第一电信号,并且基本上每个分段阴极连接到阴极电子通道,用于产生电 检测入射在半导体中的光子时的重合触发信号,第一电信号仅从与产生触发信号的阴极段相对的阳极读取。
    • 9. 发明授权
    • Optical threshold devices and methods
    • 光阈值装置和方法
    • US06892016B2
    • 2005-05-10
    • US10404077
    • 2003-04-02
    • Arie ShaharEldan Halberthal
    • Arie ShaharEldan Halberthal
    • G02B6/04G02B6/12G02B6/125G02B6/28G02B6/34G02F1/225G02F1/35H04J14/02H04J14/08G02B6/00
    • H04J14/02G02B6/04G02B6/125G02B6/2804G02B6/2861G02B2006/12107G02B2006/12142G02B2006/12145G02B2006/12147G02B2006/12164G02F1/225G02F1/3511G02F1/3523H04J14/08
    • An optical threshold device including an input, an output, first and second radiation guiding branches, each branch having first and second terminals, at least one of the first and second branches having a non-linear optical element, first and second optical couplers, at least one of the first and second optical couplers having an asymmetric optical coupler, the first optical coupler configured to split an input signal of radiation from the input into a first radiation portion propagating through the first branch and a second radiation portion propagating through the second branch, the second optical coupler configured to combine the first and second radiation portions from the second terminals of the first and second branches, respectively, into an output signal at the output, wherein the non-linear optical element produces a phase shift between the first and second radiation portions and wherein the first and second radiation portions interfere at the second coupler in response to the phase shift.
    • 一种光学阈值装置,包括输入,输出,第一和第二辐射导向分支,每个分支具有第一和第二端子,第一和第二分支中的至少一个具有非线性光学元件,第一和第二光耦合器, 所述第一和第二光耦合器中的至少一个具有不对称光耦合器,所述第一光耦合器被配置为将来自所述输入的辐射的输入信号分割成通过所述第一分支传播的第一辐射部分和通过所述第二分支传播的第二辐射部分 ,所述第二光耦合器被配置为将来自第一和第二支路的第二端子的第一和第二辐射部分分别组合成输出端的输出信号,其中非线性光学元件在第一和第二支路之间产生相移, 第二辐射部分,并且其中第一和第二辐射部分响应于第二辐射部分在第二耦合器处干扰 e相移。
    • 10. 发明授权
    • Generating of high rate modulated pulse streams
    • 生成高速调制脉冲流
    • US07567757B2
    • 2009-07-28
    • US12017363
    • 2008-01-22
    • Arie ShaharEldan Halberthal
    • Arie ShaharEldan Halberthal
    • H04J14/08
    • H04J14/08
    • All-optical system for generating high rate modulated signals. The system includes: a signal generator for generating a first periodic signal at a first rate; an optical chopping device arranged to receive the first periodic signal and to produce therefrom a second periodic signal having pulses that are narrower than the pulses of the first periodic signal; a splitting device for receiving and splitting the second periodic signal into multiple images of the second periodic signal to propagate along multiple optical paths, the multiple optical paths including optical modulators for modulating the images of the second periodic signal to produce modulated signals; and an interleaving device for receiving and interleaving the modulated signals to produce a stream of modulated signal having a second rate which is higher than the first rate.
    • 用于产生高速率调制信号的全光学系统。 该系统包括:信号发生器,用于以第一速率产生第一周期性信号; 光斩波装置被布置成接收第一周期性信号并由此产生具有比第一周期信号的脉冲窄的脉冲的第二周期信号; 分割装置,用于接收并将第二周期信号分解成多个第二周期信号的图像以沿着多个光路传播,所述多个光路包括用于调制第二周期信号的图像以产生调制信号的光调制器; 以及交织设备,用于接收和交织调制信号以产生具有高于第一速率的第二速率的调制信号流。