Abstract:
The present invention provides a charged particle optical system which emits a charged particle beam, the system including an electrostatic lens, and a grid electrode opposed to the electrostatic lens along an optical axis of the electrostatic lens, and configured to form an electrostatic field in cooperation with the electrostatic lens, wherein the grid electrode is configured such that an electrode surface, opposed to the electrostatic lens, of the grid electrode has a distance, from the electrostatic lens in a direction of the optical axis, which varies with a position in the electrode surface.
Abstract:
A shaping offset adjustment method, comprising: checking a reference point formed by an overlap of first and second shaping apertures included in a charged particle beam drawing apparatus; changing a position of the first shaping aperture by deflecting a charged particle beam so that an overlap area of the first and second shaping apertures has a predetermined shot size; measuring a current value of the charged particle beam passing through the overlap area; performing fitting on a relationship between the shot size and the corresponding current value using a cubic polynomial to calculate coefficients of the cubic polynomial achieving best fit; and correcting a shaping offset amount using the calculated coefficients of the cubic polynomial.
Abstract:
A thin flat disc with an orifice or orifices to size and control electron and other charged particulate beams. The disc is made of electrically conductive chemical vapor deposition (CVD) diamond. In addition the disc contains one or more high precision fine to ultra-fine orifices.
Abstract:
An optical encoder includes: a light source; a first grating plate having a first diffraction grating for diffracting a light beam emitted from the light source; a second grating plate having a second diffraction grating for further diffracting the light beam diffracted by the first diffraction grating; a reflector for reflecting the light beam from the second grating plate so as to allow the light beam to reenter the second grating plate; and a light-receiving portion for receiving the light beam reflected by the reflector and successively diffracted by the second and first grating plates, wherein a diffraction angle of plus and minus first-order diffracted light beams of the first diffraction grating is substantially equal to that of the plus and minus first-order diffracted light beams of the second diffraction grating, and the light-receiving portion generates an electric signal in accordance with the amount of the plus and minus first-order diffracted light beams of the first diffraction grating.
Abstract:
A charged particle optical system, e.g. an energy or mass analyzer or a lens system, has a plurality of corrector electrodes (20 to 23) spaced apart across a particle beam passing from a monoenergetic source (4) to a focus (6) and dividing the beam into individual portions with central trajectories (30,31,32) the connector electrodes being electrically biassed to deflect the particles of the beam so as to reduce the aberration caused by portions with central trajectories intersecting the optical axis at different distances from the desired focus.
Abstract:
A means is provided for compensating for spherical aberration in charged particle beam devices. The means includes a sextupole positioned between two focusing lenses.
Abstract:
A combined fine focusing micro lens array and micro deflector assembly for use in electron beam tubes of the fly's eye type is provided. The assembly comprises a fine focusing micro lens array sub-assembly formed from a plurality of spaced-apart stacked parallel thin planar apertured silicon semiconductor lens plates each having an array of micro lens aperture openings. The lens plates each have highly conductive surfaces and are secured to glass rods for holding the plates in stacked parallel spaced-apart relationship with the apertures axially aligned in parallel. A micro deflector assembly is adjacent to the micro lens array sub-assembly. A micro deflector element axially aligned with each respective fine focusing lens element serves for deflecting an electron beam passing through along orthogonal x-y directional axes of movement normal to the electron beam path. The deflector elements are comprised by two orthogonally arrayed sets of parallel spaced-apart deflector bars with alternate bars of each set of deflector bars being interconnected electrically for common connection to a respective source of fine x-y deflection potential.The thin planar apertured silicon lens plates comprising the micro lens array are held together in stacked parallel assembled relationship by spaced-apart glass support rods whose longitudinal axes extend at right angles to the plates and to which the planar silicon lens plates are secured at their periphery. The two orthogonally arrayed sets of parallel spaced-apart deflection bars forming the sets of micro-deflector elements likewise preferably comprise parallel plates or bars of polycrystalline silicon having a highly conductive metalized surface. The micro deflector bars likewise are held in assembled spaced-apart parallel relationship by respective sets of spaced-apart parallel supporting glass rods whose longitudinal axes extend in a plane parallel to the plane of the deflector bars but at right angles thereto and to which the ends of the deflector bars are thermally bonded. The fine focusing micro lens array and micro deflector sub-assembly thus comprised, are secured together in assembled relation by additional glass support rods being disposed about the outer peripheries of the micro lens and micro deflector sub-assemblies and being secured thereto by thermal bonding such as by fusion.
Abstract:
An image orthicon tube is provided with a photocathode and a target spaced therefrom. Interposed therebetween is an accelerating electrode and a further electrode interposed between the accelerating electrode and the photocathode. The accelerating electrode is supported opposite the photocathode by a distance equivalent to the longitudinal length of the further electrode. The further electrode is maintained at the same potential as that of the photocathode.