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    • 14. 发明申请
    • ELECTRODE UNIT AND CHARGED PARTICLE BEAM DEVICE
    • 电极单元和充电颗粒光束装置
    • US20110068265A1
    • 2011-03-24
    • US12992788
    • 2009-05-15
    • Noriaki AraiHideyuki Kazumi
    • Noriaki AraiHideyuki Kazumi
    • G01N23/00
    • H01J37/026H01J3/027H01J37/04H01J37/28H01J2237/0041H01J2237/0048H01J2237/30H01J2237/31749
    • A high-resolution sample image is acquired by eliminating both of charge over an entire sample (global charge) and charge in a local region irradiated with a primary charged particle beam (local charge). An electrode unit (50) according to the present invention is used in a charged particle beam device. The electrode unit (50) includes a plate electrode disposed facing an insulator sample between an objective lens and the sample, and further includes: a first charge-neutralization charged particle beam source which emits a first charged particle beam to eliminate local charge on the sample; and a second charge-neutralization charged particle beam source (25) which emits a second charged particle beam to eliminate global charge on the sample. A first hole (53) through which a primary charged particle beam passes, and a second hole through which the second charged particle beam is emitted are provided in the plate electrode, and the first and second charge-neutralization charged particle beam sources are disposed at such positions as not to interfere with each other. The charged particle beam emitted from the first charge-neutralization charged particle beam source is introduced in the vicinity of the first hole (53).
    • 通过在整个样品(全局电荷)上消除电荷并在用初级带电粒子束(局部电荷)照射的局部区域中的电荷获得高分辨率采样图像。 根据本发明的电极单元(50)用于带电粒子束装置。 电极单元(50)包括面对物镜和样品之间的绝缘体样品的平板电极,还包括:第一电荷中和带电粒子束源,其发射第一带电粒子束以消除样品上的局部电荷 ; 以及发射第二带电粒子束以消除样品上的全局电荷的第二电荷中和带电粒子束源(25)。 初级带电粒子束通过的第一孔53和第二带电粒子束发射的第二孔设置在板电极中,第一和第二电荷中和带电粒子束源设置在 这样的位置不会相互干扰。 从第一电荷中和带电粒子束源发射的带电粒子束被引入第一孔(53)附近。
    • 15. 发明授权
    • Scanning electron microscope
    • 扫描电子显微镜
    • US08698080B2
    • 2014-04-15
    • US12289461
    • 2008-10-28
    • Noriaki AraiMakoto EzumiYoichi Ose
    • Noriaki AraiMakoto EzumiYoichi Ose
    • G01N23/00
    • H01J37/026H01J37/28H01J2237/0044H01J2237/12H01J2237/2817
    • An object of the invention is to reduce the beam drift in which the orbit of the charged particle beam is deflected by a potential gradient generated by a nonuniform sample surface potential on a charged-particle-beam irradiation area surface, the nonuniform sample surface potential being generated by electrification made when observing an insulating-substance sample using a charged particle beam. Energy of the charged particle beam to be irradiated onto the sample is set so that generation efficiency of secondary electrons generated from the sample becomes equal to 1 or more. A flat-plate electrode (26) is located in such a manner as to be directly opposed to the sample. Here, the flat-plate electrode is an electrode to which a voltage can be applied independently, and which is equipped with a hole through which a primary charged particle beam can pass. Furthermore, a voltage can be applied independently to a sample stage (12) on which the sample is mounted. Here, the sample stage's surface directly opposed to the sample is formed into a planarized structure with no projections and depressions thereon. Also, diameter D of the hole provided in the flat-plate electrode (26) and distance L between the flat-plate electrode (26) and the sample are set such that a relation of D/L≦1.5 is satisfied.
    • 本发明的目的是减少带电粒子束的轨道偏转由带电粒子束照射区域表面上的不均匀样品表面电位产生的电位梯度的光束漂移,不均匀的样品表面电位为 通过使用带电粒子束观察绝缘物质样品时进行通电而产生。 设定要照射到样品上的带电粒子束的能量被设定为使得从样品产生的二次电子的产生效率等于1或更大。 平板电极(26)以与样品直接相对的方式定位。 这里,平板电极是能够独立施加电压的电极,并且具有一次带电粒子束可以穿过的孔。 此外,可以独立地对安装有样品的样品台(12)施加电压。 这里,与样品直接相对的样品台的表面形成为在其上没有凸起和凹陷的平坦化结构。 此外,设置在平板电极(26)中的孔的直径D和平板电极(26)与样品之间的距离L被设定为使得满足D / L< nlE; 1.5的关系。
    • 17. 发明申请
    • GAS FIELD IONIZATION ION SOURCE APPARATUS AND SCANNING CHARGED PARTICLE MICROSCOPE EQUIPPED WITH SAME
    • 气体放电离子源装置和扫描带有粒子的微粒显微镜
    • US20120132802A1
    • 2012-05-31
    • US13381638
    • 2010-06-08
    • Noriaki AraiTohru Ishitani
    • Noriaki AraiTohru Ishitani
    • H01J27/02H01J37/26
    • H01J27/26H01J37/023H01J37/08H01J37/28H01J2237/006H01J2237/061H01J2237/0807
    • A gas field ionization ion source apparatus is provided which is small-sized, has high-performance, and is capable of performing a tilt adjustment in a state in which an emitter tip position is maintained approximately constant. An emitter (1) is surrounded by a chamber wall (4) of an emitter chamber and ions are emitted from the tip of the emitter (1). A gas that is an ion material is introduced into the emitter chamber, through an extraction electrode (3) to which a high voltage is applied and a tube (15). The emitter (1) is cooled by a freezing means (10) through a metallic net (11) and an emitter base (12). The emitter base (12) is fixed to a movable portion (13a) of a tilting means (13). The movable portion (13a) is connected to a non-movable portion (13b) through a sliding surface (14). The sliding surface (14) forms a part of a cylindrical surface whose central axis is an axis that passes through the tip of the emitter (1) and is orthogonal to an optical axis. If the surface forms such a shape, and the amount of sliding of the sliding surface (14) is controlled, control on the tilt of the emitter (1) can be performed without moving the tip of the emitter (1).
    • 提供了一种小型化,高性能的气体电离离子源装置,并且能够在发射极尖端位置保持大致恒定的状态下进行倾斜调整。 发射器(1)被发射器室的室壁(4)包围,离子从发射器(1)的尖端发射。 作为离子材料的气体通过施加高电压的引出电极(3)和管(15)引入发射室。 发射器(1)由冷冻装置(10)通过金属网(11)和发射极基座(12)冷却。 发射极基座(12)固定在倾斜装置(13)的可动部分(13a)上。 可移动部分(13a)通过滑动表面(14)连接到不可移动部分(13b)。 滑动表面(14)形成圆柱形表面的一部分,其中心轴是穿过发射器(1)的尖端并与光轴正交的轴线。 如果表面形成这样的形状,并且控制滑动表面(14)的滑动量,则可以在不移动发射器(1)的尖端的情况下执行对发射器(1)的倾斜的控制。
    • 20. 发明申请
    • Scanning electron microscope
    • 扫描电子显微镜
    • US20070057183A1
    • 2007-03-15
    • US10566634
    • 2005-08-10
    • Noriaki AraiMakoto EzumiYoichi Ose
    • Noriaki AraiMakoto EzumiYoichi Ose
    • G21K7/00
    • H01J37/026H01J37/28H01J2237/0044H01J2237/12H01J2237/2817
    • An object of the invention is to reduce the beam drift in which the orbit of the charged particle beam is deflected by a potential gradient generated by a nonuniform sample surface potential on a charged-particle-beam irradiation area surface, the nonuniform sample surface potential being generated by electrification made when observing an insulating-substance sample using a charged particle beam. Energy of the charged particle beam to be irradiated onto the sample is set so that generation efficiency of secondary electrons generated from the sample becomes equal to 1 or more. A flat-plate electrode (26) is located in such a manner as to be directly opposed to the sample. Here, the flat-plate electrode is an electrode to which a voltage can be applied independently, and which is equipped with a hole through which a primary charged particle beam can pass. Furthermore, a voltage can be applied independently to a sample stage (12) on which the sample is mounted. Here, the sample stage's surface directly opposed to the sample is formed into a planarized structure with no projections and depressions thereon. Also, diameter D of the hole provided in the flat-plate electrode (26) and distance L between the flat-plate electrode (26) and the sample are set such that a relation of D/L≦1.5 is satisfied.
    • 本发明的目的是减少带电粒子束的轨道偏转由带电粒子束照射区域表面上的不均匀样品表面电位产生的电位梯度的光束漂移,不均匀的样品表面电位为 通过使用带电粒子束观察绝缘物质样品时进行通电而产生。 设定要照射到样品上的带电粒子束的能量被设定为使得从样品产生的二次电子的产生效率等于1或更大。 平板电极(26)以与样品直接相对的方式定位。 这里,平板电极是能够独立施加电压的电极,并且具有一次带电粒子束可以穿过的孔。 此外,可以独立地对安装有样品的样品台(12)施加电压。 这里,与样品直接相对的样品台的表面形成为在其上没有凸起和凹陷的平坦化结构。 此外,设置在平板电极(26)中的孔的直径D和平板电极(26)与样品之间的距离L被设定为使得满足D / L <1.5的关系。