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    • 3. 发明授权
    • Optical coupling to gated photocathodes
    • 光耦合到门控光电阴极
    • US06399934B1
    • 2002-06-04
    • US09642525
    • 2000-08-18
    • Jeffrey S. SullivanSteven CoyleAndres FernandezMarian Mankos
    • Jeffrey S. SullivanSteven CoyleAndres FernandezMarian Mankos
    • H01J4014
    • H01J3/024H01J37/073
    • An electron source is disclosed in which control signals having transition times less than about 10 nanoseconds and electrically isolated from a gated photocathode control an electron beam supplied by the gated photocathode. In one embodiment, the electron source includes a transmissive substrate, a photoemitter on the substrate, a gate insulator on the photoemitter, a gate electrode on the gate insulator, a housing enclosing the photoemitter and the gate electrode, a light source located outside the housing, and a detector located in the housing to receive light from the light source. The detector is electrically coupled to control a voltage applied to one of the gate electrode or the photoemitter.
    • 公开了一种电子源,其中具有小于约10纳秒的转换时间和与门控光电阴极电隔离的控制信号控制由门控光电阴极提供的电子束。 在一个实施例中,电子源包括透射衬底,衬底上的光发射器,光发射器上的栅极绝缘体,栅极绝缘体上的栅极电极,封装光电发生器和栅电极的壳体,位于壳体外部的光源 以及位于壳体中的用于接收来自光源的光的检测器。 检测器电耦合以控制施加到栅极电极或光电发射器之一的电压。
    • 5. 发明申请
    • Multiple electron beam systems
    • 多电子束系统
    • US20050264148A1
    • 2005-12-01
    • US10856111
    • 2004-05-28
    • Juan MaldonadoSteven Coyle
    • Juan MaldonadoSteven Coyle
    • H01J37/073H01J43/00H01J43/04
    • H01J37/073H01J2237/06333H01J2237/31774
    • A multiple electron beam source comprises a photon source to generate a photon beam, a lens to focus the photon beam, a photocathode having a photon receiving surface and an electron emitting surface, and an array of electron transmission gates spaced apart from the electron emitting surface of the photocathode by a distance dg. Each electron transmission gate comprises a membrane; an anode on a first surface of the membrane; an insulator on a second surface of the membrane; an aperture through the anode, insulator and membrane; and a gate electrode on the insulator. The gate electrode is positioned about the aperture and capable of receiving a gate control voltage that controls the transmission of electrons through that electron transmission gate. In one version, the multiple electron beam source comprises a photocathode stage assembly to move the photocathode relative to the array of electron transmission gates. In one version, the multiple electron beam source also comprises a plasmon-generating photon transmission plate comprising an array of photon transmission apertures and exterior surfaces capable of supporting plasmons.
    • 多电子束源包括产生光子束的光子源,聚焦光子束的透镜,具有光子接收表面和电子发射表面的光电阴极以及与电子发射表面间隔开的阵列的电子传输门 的光电阴极延伸一段距离d 。 每个电子传输门包括膜; 在膜的第一表面上的阳极; 在膜的第二表面上的绝缘体; 通过阳极,绝缘体和膜的孔; 和绝缘体上的栅电极。 栅电极围绕孔定位并且能够接收控制通过该电子传输门的电子传输的栅极控制电压。 在一个版本中,多电子束源包括相对于电子传输门阵列移动光电阴极的光电阴极级组件。 在一个版本中,多电子束源还包括等离子体发生光子传输板,其包括光子传输孔阵列和能够支撑等离子体激元的外表面。
    • 6. 发明授权
    • Current-stabilizing illumination of photocathode electron beam source
    • 光电阴极电子束源的电流稳定照明
    • US06847164B2
    • 2005-01-25
    • US10316970
    • 2002-12-10
    • Gordon JanawaySteven Coyle
    • Gordon JanawaySteven Coyle
    • H01J37/073H01J40/06
    • H01J37/073H01J2237/2817
    • An electron beam source has a photocathode with a photoemitter material having a work function, and with a beam receiving portion and an electron emitting portion. A first light source directs a first light beam onto the beam receiving portion of the photocathode to generate an electron beam from the electron emitting portion. The first light beam has a wavelength λ1 such that hc/λ1 is at least about the work function of the photoemitter material, where ‘h’ is Planck's constant and ‘c’ is the speed of light. A second light source directs a second light beam onto the beam receiving portion of the photocathode, such as onto the beam receiving portion, to stabilize the electron beam. The second light beam having a wavelength λ2 such that hc/λ2 is less than about the work function of the photoemitter material.
    • 电子束源具有具有功函数的光发射体材料的光电阴极和具有光束接收部分和电子发射部分的光电阴极。 第一光源将第一光束引导到光电阴极的光束接收部分上,以从电子发射部分产生电子束。 第一光束具有波长λ1,使得hc /λ1至少约为光电探测器材料的功函数,其中“h”为普朗克常数,“c”为光速。 第二光源将第二光束引导到光电阴极的光束接收部分,例如到光束接收部分上,以稳定电子束。 第二光束具有波长λ2,使得hc /λ2小于光发射器材料的功函数。