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    • 2. 发明授权
    • Electron beam irradiation apparatus and electron beam irradiating method
    • 电子束照射装置和电子束照射法
    • US06737660B2
    • 2004-05-18
    • US10372419
    • 2003-02-24
    • Yoshihisa MiuraYuichi AkiHiroshi KawaseMasanobu YamamotoNaoki DateSetsuo NoriokaMitsuru KoizumiGakuo Komatsubara
    • Yoshihisa MiuraYuichi AkiHiroshi KawaseMasanobu YamamotoNaoki DateSetsuo NoriokaMitsuru KoizumiGakuo Komatsubara
    • G11B910
    • H01J37/18G11B7/261H01J37/305H01J37/3056H01J2237/162H01J2237/188
    • An electron beam irradiation apparatus in a partial vacuum method is structured with a static pressure floating pad 18 connected to a vacuum chamber 14 containing an electron beam column 15 and in a condition that the static pressure floating pad 18 is attached to a subject 1 to be irradiated without contacting, and an electron beam irradiating the subject 1 to be irradiated through an electron beam path 19 of the static pressure floating pad 18, whereby the vacuum chamber and the electron beam column can be maintained in the required degree of vacuum even in a condition that the static pressure floating pad 18 is separated from the subject 1 to be irradiated. A vacuum seal valve 30 including a piston to open and close the electron beam path 19 is provided within the static pressure floating pad 18. When the static pressure floating pad 18 is separated from the subject 1, the vacuum seal valve 30 is structured to be activated to close the electron beam path 19 so as to prevent the air from flowing into the vacuum chamber 14. In this structure, the vacuum seal valve 30 is formed with a round shaped cross section and in a tapered shape with a narrow tip so as to accomplish high vacuum seal without a gap, so that the degree of vacuum in the vacuum chamber and the electron beam column can surely be maintained.
    • 部分真空法中的电子束照射装置由连接到包含电子束柱15的真空室14的静压浮动垫18构成,并且在将静压浮动垫18附着到被检体1的状态下 照射不经接触的电子束,以及通过静压浮动垫18的电子束路径19照射待被检体1的电子束,由此即使在真空室和电子束柱中也可以将真空室和电子束柱保持在所需的真空度 条件是静压浮动垫18与待照射的被检体1分离。 在静压浮动垫18内设置包括打开和关闭电子束通道19的活塞的真空密封阀30.当静压浮动垫18与被检体1分离时,真空密封阀30构成为 激活以闭合电子束路径19,以防止空气流入真空室14.在该结构中,真空密封阀30形成为圆形截面并具有窄尖端的锥形形状,以便 实现高真空密封而没有间隙,从而可以确保真空室和电子束柱中的真空度。
    • 5. 发明授权
    • Charged particle beam scanning device
    • 带电粒子束扫描装置
    • US4439681A
    • 1984-03-27
    • US312955
    • 1981-10-20
    • Setsuo NoriokaNaoki Date
    • Setsuo NoriokaNaoki Date
    • H01J37/22H01J37/24H01J37/28H04N3/22H01J37/26
    • H01J37/28H01J37/24H04N3/22
    • A charged particle beam scanning device is provided with two coordinates conversion circuits. For rotating the scanning direction of the charged particle beam, one of the coordinates conversion circuit is connected between a scanning signal generator and a magnification circuit, the output of which is supplied to a deflecting means for scanning the charged particle beam over the specimen surface, as in the case of a conventional device. Another coordinates conversion circuit is used for keeping independent operation of the image rotation and the image shift. This coordinates conversion circuit converts the output signal of a d.c. signal generator for image shift, and the converted signal is added to the input signal of the said magnification circuit.
    • 带电粒子束扫描装置设有两个坐标转换电路。 为了旋转带电粒子束的扫描方向,坐标转换电路之一连接在扫描信号发生器和放大电路之间,该放大电路的输出被提供给用于在被检体表面上扫描带电粒子束的偏转装置, 如在常规设备的情况下。 另一个坐标转换电路用于保持图像旋转和图像偏移的独立操作。 该坐标转换电路转换直流的输出信号。 用于图像偏移的信号发生器,并且将转换的信号添加到所述放大电路的输入信号。
    • 6. 发明授权
    • Method of inspecting accuracy in stitching pattern elements
    • 检查拼接图案元素精度的方法
    • US06904164B2
    • 2005-06-07
    • US09860242
    • 2001-05-18
    • Setsuo NoriokaManabu SaitoAkira Tohyama
    • Setsuo NoriokaManabu SaitoAkira Tohyama
    • G06T7/00G06K9/00G06K9/32G06K9/36
    • G06T7/001G06T7/0002G06T7/74G06T2207/30148
    • A method of quickly and accurately inspecting the stitching accuracy at which regions of a lithographic pattern are stitched at boundaries. The numerous regions of the lithographic pattern are exposed or delineated, one at a time. Inspected regions are scanned with a charged-particle beam to detect secondary electrons. The obtained signal is stored as an inspected image in an image memory, together with positional data about the inspected regions. After completion of acceptance of images from all the inspected regions, the inspected image is compared with a separately prepared reference image by an image processing unit. Pattern elements in the inspected regions corresponding to the reference image are extracted. Deviations at field boundaries or the like can be detected from the relative positions of these pattern elements, if any.
    • 快速准确地检查光刻图案的区域在边界处被缝合的缝合精度的方法。 光刻图案的许多区域被暴露或划定,一次一个。 用带电粒子束扫描检查区域以检测二次电子。 所获得的信号与检查区域的位置数据一起作为检查图像存储在图像存储器中。 在完成从所有检查区域的图像的接受之后,将检查图像与图像处理单元单独准备的参考图像进行比较。 提取与参考图像对应的被检查区域中的图案元素。 可以从这些图形元素的相对位置(如果有的话)检测场边界等的偏差。
    • 7. 发明授权
    • Electron beam instrument
    • 电子束仪器
    • US5185530A
    • 1993-02-09
    • US786264
    • 1991-11-01
    • Setsuo NoriokaHiroshi Shimada
    • Setsuo NoriokaHiroshi Shimada
    • H01J37/09
    • H01J37/09H01J2237/0264
    • A condenser means for focusing an electron beam onto a specimen and a scanning means for scanning the beam in two dimensions on the specimen placed inside a specimen chamber are disposed inside an electron beam column. The top portion of the specimem chamber is connected with the column by an annular member of a high magnetic permeability which surrounds the column. Magnetic flux passed through the top wall of the chamber is made to penetrate the annular member of a high magnetic permeability. The flux is then caused to enter the portion of the upper wall remote from the column, after which the flux leaks out. Thus, leakage of the magnetic flux into the specimem chamber is prevented.
    • 用于将电子束聚焦到样本上的聚光器装置和用于在放置在样本室内的样本上二维地扫描光束的扫描装置设置在电子束柱内。 标本室的顶部通过围绕柱的高磁导率的环形构件与柱连接。 使通过腔室顶壁的磁通量穿透高磁导率的环形构件。 然后使磁通进入远离柱的上壁的部分,之后焊剂泄漏。 因此,防止磁通量泄漏到原料室中。
    • 8. 发明授权
    • Scanning electron microscope
    • 扫描电子显微镜
    • US4990778A
    • 1991-02-05
    • US413825
    • 1989-09-28
    • Setsuo Norioka
    • Setsuo Norioka
    • H01J37/04H01J37/22H01J37/28
    • H01J37/28H01J37/222
    • In a field emission gun, current intensity of the electron beam passing through the gun anode contains a fluctuation component due to the ion bombardment and ion absorption near the emitter tip. For this reason, a scanning electron microscope having a field emission gun usually incorporates a fluctuation compensation device, which generates the signal ratio of the secondary electron signal from a specimen irradiated by the electron beam and the monitor signal corresponding to the current intensity of the electron beam passing through the gun anode and supplies the signal ratio for brightness modulation signal to the scanning image display means of the microscope. However, if the electron beam intensity is varied in a very wide operating range, the conventional fluctuation compensation device cannot operate with enough compensation effect. In this invention, the signal level of the monitor signal is maintained constant, so that the fluctuation correction device operates with enough compensation effect for a wide operating range of electron beam intensity.
    • 在场发射枪中,通过枪阳极的电子束的电流强度由于在发射极尖端附近的离子轰击和离子吸收而包含波动分量。 为此,具有场发射枪的扫描电子显微镜通常包括波动补偿装置,该波动补偿装置产生由电子束照射的样本的二次电子信号的信号比和对应于电子的当前强度的监测信号 光束通过枪阳极,并将亮度调制信号的信号比提供给显微镜的扫描图像显示装置。 然而,如果电子束强度在非常宽的工作范围内变化,则传统的波动补偿装置不能以足够的补偿效果进行工作。 在本发明中,监视信号的信号电平保持恒定,使得波动校正装置对于电子束强度的宽工作范围具有足够的补偿效果。
    • 9. 发明授权
    • Apparatus for controlling magnetic field intensity
    • 用于控制磁场强度的装置
    • US4417145A
    • 1983-11-22
    • US305404
    • 1981-09-25
    • Setsuo Norioka
    • Setsuo Norioka
    • G01N23/225G01R33/12G05F7/00H01J37/14H01J37/141H01J37/147H01J37/24H01L21/027G21K1/08H01J37/00
    • H01J37/24H01J37/14H01J37/141H01J37/1475
    • A control apparatus according to this invention is installed between an intensity specifying circuit and an excitation current source for a magnetic lens or deflecting coil. The intensity specifying circuit generates a target signal (B) corresponding to the desired magnetic flux density (B) in a magnetic lens or deflecting coil. The excitation current source outputs a current (I) which produces the desired flux density (B). Due to the effects of hysteresis the ferromagnetic yoke adjacent the lens or deflecting coil, the relationship between the target signal (B) and current (I) is nonlinear. The control apparatus has a memory in which data defining the hysteresis characteristics of the lens or coil being controlled has been stored. The control means saves the present intensity specifying signal (the old target signal) and the most recent reverse-value signal (the last target signal proceeded and followed by target signals, both of which are higher or both of which are lower than the reverse-value signal) and with the new target signal calculates the change in current (.DELTA.I) required to produce the desired flux density and commands the excitation current source to output the corresponding current. The effects due to hysteresis of the ferromagnetic yoke are dealt with by the control apparatus facilitating computer control of the electromagnetic lens or deflecting means.
    • 根据本发明的控制装置安装在用于磁性透镜或偏转线圈的强度指定电路和激励电流源之间。 强度指定电路产生与磁性透镜或偏转线圈中的期望磁通密度(B)相对应的目标信号(B)。 励磁电流源输出产生所需磁通密度(B)的电流(I)。 由于邻近透镜或偏转线圈的铁磁磁轭的滞后效应,目标信号(B)和电流(I)之间的关系是非线性的。 控制装置具有存储器,其中存储了限定被控制的透镜或线圈的滞后特性的数据。 控制装置保存当前强度指定信号(旧目标信号)和最近的反向值信号(最后的目标信号进行并跟随目标信号,两者都较高或两者均低于反向信号, 值信号),并且新的目标信号计算产生所需通量密度所需的电流变化(DELTA I),并命令激励电流源输出相应的电流。 由铁磁轭的滞后引起的影响由控制装置处理,便于计算机控制电磁透镜或偏转装置。
    • 10. 发明授权
    • Method of analyzing foreign materials
    • 异物分析方法
    • US5801382A
    • 1998-09-01
    • US889659
    • 1997-07-08
    • Osamu NodaSetsuo Norioka
    • Osamu NodaSetsuo Norioka
    • G01N23/22H01J37/256H01L21/66H01J37/00
    • H01J37/256H01J2237/2561
    • A method of quite efficiently analyzing contaminants such as dust on a semiconductor material with a scanning electron microscope. The instrument holds a list of data about contaminants. The operator selects desired items from the list and marks them to register them in a registered contaminant data table. Then, he establishes illumination conditions used for analysis and starts x-ray analysis. A secondary electron image of any contaminant of interest is displayed on a CRT at a magnification corresponding to the dimensions of the contaminant. The dimensions are retrieved from the data table. All addresses of a frame memory are searched. According to the results, the coordinates of the position of the contaminant are measured. The difference between the central position of the viewing screen of the CRT and the coordinate of the contaminant is calculated for each direction. The calculated differences are sent either to a specimen stage-driving mechanism or to an image shift power supply. In this way, the contaminant is automatically centered. The focused electron beam is directed at the center of this contaminant to produce x-rays. If the analysis of this wafer is not yet complete, data about the next contaminant item is retrieved from the registered contaminant data table.
    • 用扫描电子显微镜相当有效地分析半导体材料上的灰尘等污染物的方法。 该仪器包含有关污染物的数据列表。 操作员从列表中选择所需的项目,并将其标记为在注册的污染物数据表中注册。 然后,他建立了用于分析的照明条件,开始X射线分析。 感兴趣的任何污染物的二次电子图像以与污染物的尺寸相对应的放大倍数显示在CRT上。 从数据表中检索尺寸。 搜索帧存储器的所有地址。 根据结果​​,测量污染物位置的坐标。 对于每个方向计算CRT的观察屏幕的中心位置和污染物的坐标之间的差异。 将计算出的差异发送到样本台驱动机构或图像移位电源。 以这种方式,污染物自动居中。 聚焦的电子束被引导到该污染物的中心以产生x射线。 如果该晶片的分析尚未完成,则从登记的污染物数据表中检索关于下一污染物项目的数据。