Abstract:
In order to provide a method to easily and surely adjust the focal distance as in a Wobbler apparatus of the transmission type electron microscope method, a crossover 11 of a charged particle beam 2 is established between a charged particle gun 1 and an objective lens 6 and a beam deflection device 4 is provided to deflect the charged particle beam at the crossover point as the supporting point. A total controller 9 calculates an amount of the out of focus from a moving amount of the microscopic image obtained by deflecting the beam and orders the objective lens power supply to move the microscopic image as the focal distance.
Abstract:
The invention relates to a particle-optical apparatus for particle-optical mask projection. According to the invention, an energy filter is used, by which particles which are inelastically scattered in a mask plane are separated from particles which are elastically scattered in the mask plane. Particles from a selected energy range are used for the particle-optical imaging of the mask in the final image plane. The energy filter is an imaging energy filter, the mask plane being coincident with the input image plane of the energy filter or being imaged in it. The output image plane of the energy filter is imaged, reduced in scale, by a following imaging system on a wafer arranged in the projection plane. Beam deflection systems are provided in addition, by which the particle beam is deflectable in the mask plane and onto out-of-axis regions, so that different regions of the mask plane can be imaged in the image plane at successive times.
Abstract:
According to a known projection lithography method an object is imaged on an imaging surface by means of a telescopic system of rotationally symmetrical electron lenses. The throughput during the production of integrated circuits by means of projection lithography is determined by the amount of current in the imaging electron beam; this current is limited by the resolution-limiting interaction of the electrons (Coulomb interaction). The invention allows for a larger beam current in that areas with a high current concentration are avoided. To this end, the imaging system includes five mutually perpendicular quadrupoles, so that the electrons are concentrated in line-shaped focal spots instead of a (small) circular cross-over. The system is telescopic and the imaging is stigmatic with equal magnifications in the x-z plane and the y-z plane.
Abstract:
particle-optical apparatus at a comparatively low acceleration voltage (from 0.5 kV to 5 kV). This lens defect cannot be eliminated by means of rotationally-symmetrical fields. In order to enhance the resolution nevertheless, it has already been proposed to mitigate said lens defect by means of a corrector of the Wien type. This known configuration consists of a number of electrical and magnetic multipoles. In order to adapt the corrective capacity of the corrector 28 to the strength of the objective 8 to be corrected and to achieve less severe requirements in respect of mechanical tolerances, according to the invention the corrector 28 is excited in such a manner that the trajectory of the electrons constitutes a sinusoid of a length which does not deviate more than 10% from a full sine period, upstream and downstream from the correction device there being arranged an n-pole, where n=4, 6, . . . (27, 29), at a distance which is less than ¼ of the length of the corrector.
Abstract:
According to a known projection lithography method an object is imaged on an imaging surface by means of a telescopic system of rotationally symmetrical electron lenses. The throughput during the production of integrated circuits by means of projection lithography is determined by the amount of current in the imaging electron beam; this current is limited by the resolution-limiting interaction of the electrons (Coulomb interaction). The invention allows for a larger beam current in that areas with a high current concentration are avoided. To this end, the imaging system includes five mutually perpendicular quadrupoles, so that the electrons are concentrated in line-shaped focal spots instead of a (small) circular cross-over (18). The system is telescopic and the imaging is stigmatic with equal magnifications in the x-z plane and the y-z plane.