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    • 3. 发明授权
    • Variable axis stigmator
    • 可变轴标枪
    • US5389858A
    • 1995-02-14
    • US915798
    • 1992-07-16
    • Guenther O. LangnerPaul F. Petric
    • Guenther O. LangnerPaul F. Petric
    • H01J29/76H01J37/141H01J37/153H01J37/30H01J37/305G09G1/04G21K1/08H01J3/14
    • H01J37/141H01J37/153H01J37/3007
    • The magnetic axis of a stigmation yoke is varied from the mechanical axis of the stigmation yoke by differentially driving pairs of coils in a quadrupole configuration with currents which differ from a nominal stigmation current by approximately equal amounts, applied in opposite senses. Set-up procedures for electron beam deflection systems, such as in e-beam tools, are automated by emulating manual procedures in combination with electrical alteration of the magnetic axis of the stigmator yoke. Stigmation errors can also be corrected under automated set-up procedure control to allow dynamic correction of astigmatism in electron beam deflection system. Electrically variability of the magnetic axis of the stigmator yoke also allows the placement of the stigmator yoke at a position in the electron optical column other than prior to deflection stages as well as improved freedom from positional and aberrational errors.
    • 通过在四极配置中差分驱动成对的线圈,通过以相反的方向施加大约相等量的标称标称电流的电流差异地驱动柱形磁轭的机械轴线,磁极轴的磁轴是从机械轴线变化的。 用于电子束工具的电子束偏转系统的设置程序通过模拟手动程序与喷枪轭的磁轴的电气改变相结合而自动化。 在自动设置程序控制下也可以纠正标示误差,以​​允许电子束偏转系统中的散光动态校正。 柱状磁轭的磁轴的电气变化也允许将标称磁轭放置在电子光学柱的位置之外,而不是在偏转阶段之前的位置以及改进的位置和像差误差的自由度。
    • 4. 发明授权
    • Method for measurement of spotsize and edgewidth in electron beam
lithography
    • 电子束光刻中斑点和边缘的测量方法
    • US4675528A
    • 1987-06-23
    • US750081
    • 1985-06-28
    • Guenther O. LangnerKenneth J. HarteMichael J. DalterioMarvin Fishbein
    • Guenther O. LangnerKenneth J. HarteMichael J. DalterioMarvin Fishbein
    • G01B15/00G01Q20/00H01J37/28G01N27/00
    • H01J37/28G01B15/00
    • The technique of measuring the spotsize and edgewidth of an electron beam by incrementally scanning the beam through discrete scan locations across a sharp edge is improved by processing the resulting beam current signals directly rather than the differentiated beam current signal. A linear regression is performed on beam current data points expected to fall in the linear portion of the beam current versus beam position characteristic in order to provide a linear approximation of the overall characteristic. Extrapolation of the linear function to its intersections with the maximum (I.sub.1) and minimum (I.sub.0) beam current levels yields corresponding beam positions Z.sub.B and Z.sub.A, such that (Z.sub.B -Z.sub.A) is a measure of spotsize in the scan direction. Edgewidth between the twelve and eighty-eight percent amplitude levels is obtained by locating measured beam currents at incremental scan locations on both sides of beam positions Z.sub.A and Z.sub.B, and interpolating to find the actual beam currents I.sub.A and I.sub.B at these positions. Edgewidths D.sub.A and D.sub.B are computed as D.sub.A =4.sqroot..pi.(Z.sub.B -Z.sub.A)(I.sub.A -I.sub.0)(I.sub.1 -I.sub.0) and D.sub.B =4.sqroot..pi.(Z.sub.B -Z.sub.A)(I.sub.1 -I.sub.B)(I.sub.1 -I.sub.0). In the case of a square beam with rounded corners, spotsize (i.e., side of square) is measured by a diagonal incremental scan and determination, by interpolation, of the beam positions Z.sub.C and Z.sub.D at which the beam current is I.sub.C =I.sub.0 +19(I.sub.1 -I.sub.0)/64 and I.sub.D =I.sub.0 +45(I.sub.1 -I.sub.0)/64. The spotsize is then computed from the formula 3.01816 (Z.sub.C -Z.sub.D).
    • 通过跨越尖锐边缘通过离散扫描位置逐渐扫描光束来测量电子束的斑点和边缘的技术通过直接处理所得到的束电流信号而不是分化的束电流信号来改进。 对预期落入光束电流与光束位置特性的线性部分的光束电流数据点进行线性回归,以提供整体特性的线性近似。 将线性函数外推到具有最大(I1)和最小(I0)光束电流水平的交点产生相应的光束位置ZB和ZA,使得(ZB-ZA)是扫描方向上的斑点的量度。 通过将测量的束电流定位在光束位置ZA和ZB的两侧上的增量扫描位置,并进行内插以在这些位置处找到实际的光束电流IA和IB,可以获得十八至八十八%的幅度电平之间的宽度。 EDG宽度DA和DB计算为DA = 4 2ROOT pi(ZB-ZA)(IA-I0)(I1-I0)和DB = 4 2ROOT pi(ZB-ZA)(I1-IB)(I1-I0)。 在具有圆角的方束的情况下,通过对角线增量扫描来测量斑点(即,平方的一侧),并且通过插值来确定束电流为IC = I0 + 19的光束位置ZC和ZD (I1-I0)/ 64和ID = I0 + 45(I1-I0)/ 64。 然后从公式3.01816(ZC-ZD)计算斑点。
    • 7. 发明授权
    • Variable axis electron beam projection system
    • 变轴电子束投影系统
    • US4376249A
    • 1983-03-08
    • US204427
    • 1980-11-06
    • Hans C. PfeifferGuenther O. LangnerMaris A. Sturans
    • Hans C. PfeifferGuenther O. LangnerMaris A. Sturans
    • H01J37/141H01J37/147H01J37/153H01J37/30H01J3/20
    • H01J37/3007H01J37/1474
    • An electron beam projection system having a projection lens arranged so that upon pre-deflection of the electron beam the electron optical axis of the lens shifts to be coincident with the deflected beam. The projection system includes means for producing an electron beam, means for deflecting the beam, a magnetic projection lens having rotational symmetry for focusing the deflected beam and a pair of magnetic compensation yokes positioned within the bore of the projection lens means. The pair of correction yokes has coil dimensions such that, in combination, they produce a magnetic compensation field proportional to the first derivative of the axial magnetic field strength distribution curve of the projection lens. Upon application of current to the pair of compensation yokes the electron optical axis of the projection lens shifts to the position of the deflected beam so that the electron beam remains coincident with the shifted electron optical axis and lands perpendicular to a target.
    • 一种具有投影透镜的电子束投影系统,其布置成使得在电子束的预偏转时,透镜的电子光轴移动以与偏转光束重合。 投影系统包括用于产生电子束的装置,用于偏转光束的装置,具有用于聚焦偏转光束的旋转对称性的磁性投影透镜和位于投影透镜装置的孔内的一对磁性补偿轭。 一对校正轭具有线圈尺寸,使得它们组合地产生与投影透镜的轴向磁场强度分布曲线的一阶导数成比例的磁补偿场。 在将电流施加到一对补偿轭时,投影透镜的电子光轴移动到偏转光束的位置,使得电子束与移动的电子光轴保持一致并垂直于目标。