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    • 62. 发明授权
    • Charged particle beam orbit corrector and charged particle beam apparatus
    • 带电粒子束轨道校正器和带电粒子束装置
    • US07947964B2
    • 2011-05-24
    • US11943241
    • 2007-11-20
    • Hiroyuki ItoYuko SasakiTohru IshitaniYoshinori Nakayama
    • Hiroyuki ItoYuko SasakiTohru IshitaniYoshinori Nakayama
    • G21K1/087
    • H01J37/141H01J37/09H01J37/12H01J37/153H01J37/28H01J2237/142H01J2237/1534H01J2237/303
    • The present invention relates to an orbit correction method for a charged particle beam, and aims to solve problems inherent in conventional aberration correction systems and to provide a low-cost, high-precision, high-resolution optical converging system for a charged particle beam. To this end, employed is a configuration in which a beam orbit is limited in ring zone form to form a distribution of electromagnetic field converging toward the center of a beam orbit axis. Consequently, a nonlinear action outwardly augmented, typified by spherical aberration of an electron lens, can be cancelled out. Specifically, this effect can be achieved by an electron disposed on the axis and subjected to a voltage to facilitate the occurrence of electrostatic focusing. For a magnetic field, this effect can be achieved by forming a coil radially distributed-wound on a surface equiangularly divided in the direction of rotation to control convergence of a magnetic flux density.
    • 本发明涉及一种用于带电粒子束的轨道校正方法,其目的在于解决常规像差校正系统中固有的问题,并提供一种用于带电粒子束的低成本,高精度,高分辨率的聚光系统。 为此,所采用的是波束轨道受环形形式限制以形成朝向光束轨道中心收敛的电磁场分布的结构。 因此,可以抵消以电子透镜的球面像差为代表的向外扩大的非线性动作。 具体地说,这种效果可以通过设置在轴上的电子元件实现,并且经受电压以便于静电聚焦的发生。 对于磁场,这种效果可以通过在旋转方向上等角地分割的表面上形成径向分布缠绕的线圈来实现,以控制磁通密度的收敛。
    • 63. 发明授权
    • Focused ION beam apparatus
    • 聚焦光束装置
    • US07550740B2
    • 2009-06-23
    • US11828714
    • 2007-07-26
    • Koichiro TakeuchiTohru Ishitani
    • Koichiro TakeuchiTohru Ishitani
    • G21K1/093H01J29/58H01J29/64H01J37/21
    • H01J37/3056H01J37/09H01J37/1471H01J2237/31745H01J2237/31749
    • A focused ion beam apparatus enables an ion beam to be focused highly accurately on a sample at the beam spot position of the case of the absence of magnetic field without causing isotope separation of the ion beam on the sample, even when there is a magnetic field on the ion beam optical axis or the magnetic field fluctuates. The focused ion beam apparatus comprises a corrective magnetic field generating unit 10 disposed on the optical axis of the ion beam 3 for correcting the deflection of the ion beam 3 due to an external magnetic field. The corrective magnetic field generating unit 10 includes pole-piece pairs 26A and 26B, each of which having two pole pieces 26a and 26b or 26c and 26d that are adjacent to each other with a gap d. The pole-piece pairs 26A and 26B are disposed opposite to each other with a gap g (>d) across the optical axis of the ion beam 3. Each of the pole pieces 26a to 26d is wound with an internal coil 29, and the pole-piece pairs 26A and 26B are each wound with an external coil 30 in such a manner as to surround the internal coils 29.
    • 聚焦离子束装置使得离子束能够在不存在磁场的情况下的光束位置处的样品上高精度地聚焦,而不会导致样品上的离子束同位素分离,即使存在磁场 在离子束光轴上或磁场波动。 聚焦离子束装置包括设置在离子束3的光轴上的校正磁场产生单元10,用于校正由外部磁场引起的离子束3的偏转。 校正磁场产生单元10包括极片对26A和26B,每个具有间隙d彼此相邻的两个极片26a和26b或26c和26d。 极片对26A和26B彼此相对地设置有跨越离子束3的光轴的间隙g(> d)。每个极片26a至26d都缠绕有内部线圈29,并且 极片对26A和26B分别以包围内部线圈29的方式缠绕有外部线圈30。
    • 64. 发明申请
    • Liquid metal ion gun
    • 液态金属离子枪
    • US20080210883A1
    • 2008-09-04
    • US12076481
    • 2008-03-19
    • Hiroyasu KagaYuichi MadokoroShigeru IzawaTohru IshitaniKaoru Umemura
    • Hiroyasu KagaYuichi MadokoroShigeru IzawaTohru IshitaniKaoru Umemura
    • G21G5/00
    • H01J27/02H01J27/22H01J37/08H01J2237/0805
    • An emitter of a Ga liquid metal ion source is constituted to include W12 of a base material and Ga9 of an ion source element covering a surface as construction materials. By making back-sputtered particles become elements (W and Ga) of the Ga liquid metal ion sour source, if back-sputtered particles attach to the Ga liquid metal ion source, contamination which may change physical characteristics of Ga9 does not occur. A W aperture is used as a beam limiting (GUN) aperture to place Ga of approx. 25 mg (of melting point of 30° C.) on a surface of a portion included in a beam emission region (Ga store). When emitting ions to the beam limiting (GUN) aperture, Ga in the emission region melts and diffuses on a surface of the beam emission region of the W aperture.
    • Ga液体金属离子源的发射极构成为包括基材的W12和覆盖表面的离子源元素的Ga9作为构造材料。 通过使反溅射的颗粒成为Ga液态金属离子源的元素(W和Ga),如果反溅射的颗粒附着到Ga液态金属离子源,则不会发生可能改变Ga9的物理特性的污染物。 使用W光圈作为光束限制(GUN)光圈来放置大约的Ga。 在束发射区域(Ga储存)中包含的部分的表面上25mg(熔点为30℃))。 当将离子发射到光束限制(GUN)孔径时,发射区域中的Ga在W光阑的束发射区域的表面上熔化并扩散。
    • 67. 发明授权
    • Liquid metal ion gun
    • 液态金属离子枪
    • US07211805B2
    • 2007-05-01
    • US11312367
    • 2005-12-21
    • Hiroyasu KagaYuichi MadokoroShigeru IzawaTohru IshitaniKaoru Umemura
    • Hiroyasu KagaYuichi MadokoroShigeru IzawaTohru IshitaniKaoru Umemura
    • H01J27/00G21G5/00G21K7/00
    • H01J27/02H01J27/22H01J37/08H01J2237/0805
    • An emitter of a Ga liquid metal ion source is constituted to include W12 of a base material and Ga9 of an ion source element covering a surface as construction materials. By making back-sputtered particles become elements (W and Ga) of the Ga liquid metal ion sour source, if back-sputtered particles attach to the Ga liquid metal ion source, contamination which may change physical characteristics of Ga9 does not occur. A W aperture is used as a beam limiting (GUN) aperture to place Ga of approx. 25 mg (of melting point of 30° C.) on a surface of a portion included in a beam emission region (Ga store). When emitting ions to the beam limiting (GUN) aperture, Ga in the emission region melts and diffuses on a surface of the beam emission region of the W aperture.
    • Ga液体金属离子源的发射极构成为包括基材的W12和覆盖表面的离子源元素的Ga9作为构造材料。 通过使反溅射的颗粒成为Ga液态金属离子源的元素(W和Ga),如果反溅射的颗粒附着到Ga液态金属离子源,则不会发生可能改变Ga9的物理特性的污染物。 使用W光圈作为光束限制(GUN)光圈来放置大约的Ga。 在束发射区域(Ga储存)中包含的部分的表面上25mg(熔点为30℃))。 当将离子发射到光束限制(GUN)孔径时,发射区域中的Ga在W光阑的束发射区域的表面上熔化并扩散。