摘要:
An automatic focus correction system for E-beam lithography uses optical light from a narrow angle light source to illuminate a horizontal slit, the image of which is projected onto a target surface. Prior to and after reflection of the slit image from the target surface the light beam is projected parallel to the target surface to minimize vertical space requirements in the E-beam column. Variations in height, z-position, cause the slit image to move vertically and the focus of reflection to shift laterally and this image is redeflected in the horizontal plane by a prism to a linear diode array used to produce a video-type output signal. Autofocus electronics are used to convert the video output signal into an analog correction signal to the E-beam fine focus coil. The video-type signal is also converted to a digital height value to be used for corrections in beam magnification and rotation.
摘要:
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.
摘要:
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).
摘要:
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.
摘要:
An improved particle lens has an axis that is shifted to follow the central ray of the beam as it is deflected through the lens creating, in effect, a variable curvilinear optical axis for the lens and introducing aberrations depending on the object size and the distance off the lens symmetry axis. These aberrations are corrected by a set of wire pairs perpendicular to the system axis to add a gradient of the z-component of the magnetic field by which aberrations are generated of the same type but opposite direction as those inherent in the system.
摘要:
A dynamic correction arrangement for an electron beam projection/deflection system provides high order correction values for deflection in accordance with a correction equation. Particularly as applied to high accuracy telecentric deflection, the coefficients of terms of the correction equation may be determined by calibration for a small number of test points. Correction values may be stored in a look-up table or computed in real time by using a math co-processor in a processing pipeline. The correction provided corrects landing angle errors through the third order in telecentric projection/deflection systems such as systems utilizing variable axis immersion lenses.
摘要:
An improved particle lens has an axis that is shifted to follow the central ray of the beam as it is deflected through the lens creating, in effect, a variable curvilinear optical axis for the lens and introducing aberrations having depending on the object size and the distance off the lens symmetry axis. These aberrations are corrected by a set of correction elements generating compensating aberrations of the same type, comprising at least one wire pair perpendicular to the system axis and carrying fixed currents to introduce a gradient in the field, together with three coils centered on the system axis to cancel a bias field introduced by the wire pair.
摘要:
A scanned electron beam system employs an electron beam source using an NEA activated photo-emitter as the cathode. The activated photo-emitter cathode produces a pre-shaped electron beam having a relatively small spot focussed on a target plane. The beam is selectively deflected to scan the beam spot along the target plane to expose desired patterns on that plane. The distance between the cathode and anode can be made large enough to accommodate in situ replenishment of cathode material, such as Cesium, without obstructing the electron optical path. The system includes two vacuum chambers which are differentially pumped through respective ports. The first chamber, in which the anode and cathode are located, is utilized for establishing the required electrostatic field. The second chamber is employed to produce the necessary focussing and selective beam deflection.
摘要:
An all-electrostatic variable spot charged particle (electron) beam shaping sub-system which is compact and of much smaller size than known similar systems designed for the same purpose and operating with magnetic lenses. The improved electrostatic variable spot-shaping sub-system does not require mechanical rotation of the spot-shaping apertures for maintaining alignment or orientation. The improved sub-system includes both beam steering and beam blanking requiring less than 3 volts for operation of the blanking controls to turn the beam on and off. The novel system easily accomodates a variety of different beam-shaping apertures for use as the second beam shaping aperture in the sub-system including rectilinear triangles of different orientation to provide smooth 45 degree pattern delineation, rectangles, squares, and even different diameter circles where such configurations are required by a particular pattern to be written in the target plane.
摘要:
A charged particle lens has an axis that is shifted to follow the central ray of the beam as it is deflected through the lens creating, in effect, a variable curvilinear optical axis for the lens and introducing aberrations having depending on the object size and the distance off the lens symmetry axis. These aberrations are corrected by a set of coil pairs tilted with respect to the system axis, which generate compensating aberrations of the same type.