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    • 86. 发明公开
    • Source for intense coherent electron pulses
    • 强化,kohärentegepulste Elektronenquelle。
    • EP0563500A1
    • 1993-10-06
    • EP92810245.8
    • 1992-04-01
    • International Business Machines Corporation
    • Fink, Hans-Werner, Dr.Schmid, Heinz
    • H01J37/073H01J3/02
    • H01J3/021H01J37/073
    • This source for intense coherent electron pulses of an energy below 1 keV comprises an ultrasharp electron-emitting tip (10) and an anode (11), both arranged in mutual alignment inside a vacuum envelope (9). A pulsed potential with an amplitude in the range between 100 V and 500 V and with a variable pulse rate is applied between said tip (10) and said anode (11). The tip (10) is maintained negative with respect to said anode (11), the tip (10) having a sharpness such that the electric field at its surface exceeds 10⁷ V/cm at said pulsed potential.
      An object (14) is arranged downstream in front of the opening (12) in said anode (11) within the electron beam, such that the spherical wave of electrons arriving at a screen (13) arranged opposite said tip (10) and oriented orthogonally with respect to the axis of the electron beam passing said opening (12), generates an interference pattern thereon, namely a Gabor hologram in case said object (14) is smaller than the diameter of said opening (12), and a transmission hologram in the case said object (14) is bigger than the diameter of said opening (12) and at least partially transparent to the electron beam.
    • 这种用于低于1keV的能量的强相干电子脉冲的源包括超真空电子发射尖端(10)和阳极(11),两者均布置成在真空外壳(9)内相互对准。 在所述尖端(10)和所述阳极(11)之间施加振幅在100V和500V之间并且具有可变脉冲速率的脉冲电位。 尖端(10)相对于所述阳极(11)保持为负极,尖端(10)具有清晰度,使得其表面处的电场在所述脉冲电势处超过10V / cm。 物体(14)被布置在电子束内的所述阳极(11)的开口(12)的前方的下游,使得到达与所述尖端(10)相对布置的屏幕(13)的电子球形波取向 相对于通过所述开口(12)的电子束的轴线正交地,在所述物体(14)小于所述开口(12)的直径的情况下,在其上产生干涉图案,即Gabor全息图,以及透射全息图 在所述物体(14)大于所述开口(12)的直径并且对于电子束至少部分透明的情况下。
    • 88. 发明公开
    • A field emission device and method for forming
    • Feldemissionsvorrichtung und Verfahren zur Herstellung。
    • EP0523980A1
    • 1993-01-20
    • EP92306481.0
    • 1992-07-15
    • MOTOROLA, INC.
    • Kane, Robert C.Hilgers, Kevin B.
    • H01J9/02H01J1/30
    • H01J3/021H01J1/3042H01J9/025
    • A method of producing an FED including a central conductive region (103) having a surface perpendicular to the supporting structure (101) forming a device anode, a structure including first (106) and second (112) layers.of intrinsic semiconductor material with a conductive layer (105), forming an emitter, sandwiched therebetween and stacked to each provide a surface parallel to and spaced from the conductive region (103) surface, and conductive layers (114) disposed on the provided surfaces of the first (106) and second 9112) layers, perpendicular to the sandwiched conductive layer (105), in spaced relation to each other and the sandwiched conductive layer (105) to form gate extraction electrodes.
    • 一种制造FED的方法,包括具有垂直于形成器件阳极的支撑结构(101)的表面的中心导电区(103),包括本征半导体材料的第一(106)和第二(112)层的结构,其具有 导电层(105),形成发射极,夹在它们之间并且层叠以提供与导电区域(103)表面平行并与之隔开的表面,以及布置在第一(106)的所提供的表面上的导电层(114)和 垂直于夹层导电层(105)的第二层9112)彼此间隔开并且夹持导电层(105)形成栅极引出电极。
    • 90. 发明公开
    • Electron emitting structure and manufacturing method
    • 电子发射结构与制造方法
    • EP0501785A3
    • 1992-11-19
    • EP92301632.3
    • 1992-02-26
    • RAYTHEON COMPANY
    • Feist, Wolfgang M.
    • H01J1/30H01J17/49H01J9/02
    • H01J9/025H01J3/021H01J31/127H01J2329/8625
    • A field emitter includes an electron emitting structure (112) spaced from an anode structure (114), with the intervening gap (113) being substantially evacuated. The electron emitting structure (112) includes a first electrically conductive layer (128) spaced by an insulating layer (130) from a second conductive layer (132), and a generally circular aperture (134) disposed through the layers (128,132). The anode structure (114) includes an electrically conductive layer (142). Electrostatic forces, provided from a potential applied between the first conductive layer (128) and the anode structure (114), cause an electron beam to be drawn from a cathode provided by a peripheral edge portion (127a) of the first conductive layer (128) within the aperture (134) onto an adjacent surface portion of the anode structure (114). Such field emission occurs under the control of a potential applied between the first and second conductive layers (128,132) of the electron emitting structure with the second conductive layer (132) functioning as a control electrode of the emitting structure. The anode structure (114) has a phosphor layer (144) which converts the electrical energy from the electron bombardment into visible light energy. In one embodiment (Fig. 6), a potential applied to a third conductive layer (360) of the emitting structure (312) serves to focus the electron stream on the anode structure (314). Methods of manufacturing the electron emitting structures employ successive steps of layer deposition and subsequent selective etching.
    • 场致发射器包括与阳极结构(114)间隔开的电子发射结构(112),其间隙(113)基本上被抽空。 电子发射结构(112)包括由绝缘层(130)与第二导电层(132)间隔开的第一导电层(128)和穿过层(128,132)设置的大致圆形孔(134)。 阳极结构(114)包括导电层(142)。 从施加在第一导电层(128)和阳极结构(114)之间的电位提供的静电力使得电子束从由第一导电层(128)的外围边缘部分(127a)提供的阴极被拉伸 )到阳极结构(114)的相邻表面部分上。 这种场发射在施加在电子发射结构的第一和第二导电层(128,132)之间的电位的控制下发生,而第二导电层(132)用作发光结构的控制电极。 阳极结构(114)具有将电子轰击的电能转换为可见光能的荧光体层(144)。 在一个实施例(图6)中,施加到发光结构(312)的第三导电层(360)的电位用于将电子流聚焦在阳极结构(314)上。 制造电子发射结构的方法采用层沉积和随后的选择性蚀刻的连续步骤。