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    • 4. 发明授权
    • Charged particle beam device and filter member
    • 带电粒子束装置和过滤元件
    • US09373480B2
    • 2016-06-21
    • US14782695
    • 2014-03-05
    • Hitachi High-Technologies Corporation
    • Shinsuke KawanishiYusuke OminamiMasahiko AjimaHiroyuki Suzuki
    • H01J37/16H01J37/18H01J37/20H01J37/02H01J37/26
    • H01J37/16H01J37/026H01J37/18H01J37/20H01J37/26H01J2237/0213H01J2237/022H01J2237/2003H01J2237/2006
    • In a SEM device which enables observations under an atmospheric pressure, in the event that a diaphragm is damaged during an observation of a sample, air flows into a charged particle optical barrel from the vicinity of the sample, due to the differential pressure between the inside of the charged particle optical barrel under vacuum and the vicinity of the sample under the atmospheric pressure. At this time, the sample may be sucked into the charged particle optical barrel. In this case, a charged particle optical system and a detector are contaminated thereby, which causes performance degradation or failures of the charged particle microscope. For coping therewith, it is necessary to prevent the charged particle optical barrel from being contaminated, without inducing a time lag, with a simple structure. In a charged particle beam device adapted to place a sample in a non-vacuum environment, there is provided a filter member which is placed on the path of a primary charged particle beam at least in a state where the primary charged particle beam is directed to the sample and, further, is adapted to transmit or pass, therethrough, the primary charged particle beam and secondary charged particles derived from the sample, while intercepting at least a portion of a scattering substance which is scattered in the event of a fracture of the diaphragm.
    • 在能够在大气压下进行观察的SEM装置中,在样品观察期间膜片损伤的情况下,由于内部的压差,空气从样品附近流入带电粒子光学镜筒 的带电粒子光学筒在真空下和样品在大气压附近。 此时,样品可以被吸入带电粒子光学筒中。 在这种情况下,带电粒子光学系统和检测器被污染,导致带电粒子显微镜的性能下降或失效。 为了应对,需要以简单的结构防止带电粒子光学筒被污染,而不会引起时间滞后。 在适于将样品置于非真空环境中的带电粒子束装置中,设置有过滤构件,其至少在初级带电粒子束被引导到 样品,并且还适于透射或通过从样品衍生的初级带电粒子束和二次带电粒子,同时截留至少一部分在发生断裂的情况下散射的散射物质 隔膜
    • 6. 发明授权
    • Method for providing uniform distribution of plasma density in a plasma treatment apparatus
    • 在等离子体处理装置中提供等离子体密度均匀分布的方法
    • US09275840B2
    • 2016-03-01
    • US14164179
    • 2014-01-25
    • Yuri Glukhoy
    • Yuri Glukhoy
    • H01J37/32B05D7/22C23C14/08C23C16/40
    • H01J37/32449B05D7/22C23C14/083C23C16/405H01J37/32091H01J37/32477H01J37/32807H01J2237/0213H01J2237/04Y10T29/4998
    • Proposed is a method for providing uniform distribution of plasma density in a CCP plasma processing apparatus. According to the method the through gas holes of the showerhead of used in the plasma processing chamber of the apparatus are provided with conical nozzles formed on the side of the gas holes that face the gas reservoir of the cooler plate. The cone angle θ of the nozzles decreases in the direction from the peripheral portion to the central area of the showerhead in the range from 120° to 0°. Since the conical nozzles increase the gas gap between the showerhead and the cooler plate, more favorable conditions are created for electric breakdown. In order to protect the surfaces of the conical nozzles and gas holes from deterioration by hollow cathode discharge, these surface are coated by a protective coating resistant to electrical breakdown and chemical corrosion.
    • 提出了一种在CCP等离子体处理装置中提供等离子体密度均匀分布的方法。 根据该方法,在装置的等离子体处理室中使用的喷头的通气孔设置有形成在与冷却器板的气体储存器相对的气孔侧的锥形喷嘴。 锥角与角度; 的喷嘴在从120°至0°的范围内从喷墨头的周边部分到中心区域的方向上减小。 由于锥形喷嘴增加了淋浴头和冷却板之间的气隙,因此为电击穿创造了更有利的条件。 为了保护锥形喷嘴和气孔的表面免受空心阴极放电的损坏,这些表面涂有耐电击穿和化学腐蚀的保护涂层。
    • 7. 发明申请
    • ION IRRADIATION DEVICE AND ION IRRADIATION METHOD
    • 离子辐照装置和离子辐射方法
    • US20160013011A1
    • 2016-01-14
    • US14833533
    • 2015-08-24
    • ULVAC, Inc.
    • Takumi YUZEToshihiro TERASAWA
    • H01J37/04
    • H01J37/04H01J37/09H01J37/1472H01J37/3171H01J2237/0213H01J2237/028H05H1/16H05H7/04
    • Positive ions that fly within an ion acceleration tube are accelerated by a plurality of acceleration electrodes arranged within the ion acceleration tube and are irradiated to an irradiation target. A plurality of magnet devices is arranged within the ion acceleration tube; the directions of the lines of magnetic force formed respectively by the magnet devices are made to differ between the adjacent magnet devices by an angle of more than 0 degree and at most 90 degrees or less; and each of the lines of magnetic force is rotated in one direction within the ion acceleration tube. Electrons travelling in reverse within the ion acceleration tube are made to intersect the lines of magnetic force, and made to increase a distance from a flying axis while traveling in reverse. Since the electrons collide with members within the ion acceleration tube and stop before having high energy, high-energy X-rays are not generated.
    • 在离子加速管内飞行的正离子被布置在离子加速管内的多个加速电极加速并照射到照射目标。 多个磁体装置设置在离子加速管内; 使磁铁装置分别形成的磁力线的方向在相邻的磁体装置之间的角度大于0度,最大为90度以下; 并且每个磁力线在离子加速管内沿一个方向旋转。 使离子加速管内的相反行进的电子与磁力线相交,并且在相反行进时增加与飞行轴的距离。 由于电子与离子加速管内的构件碰撞并且在具有高能量之前停止,所以不产生高能X射线。