Abstract: A charged particle system comprises a particle source for generating a beam of charged particles and a particle-optical projection system. The particle-optical projection system comprises a focusing first magnetic lens (403) comprising an outer pole piece (411) having a radial inner end (411?), and an inner pole piece (412) having a lowermost end (412?) disposed closest to the radial inner end of the outer pole piece, a gap being formed by those; a focusing electrostatic lens (450) having at least a first electrode (451) and a second electrode (450) disposed in a region of the gap; and a controller (C) configured to control a focusing power of the first electrostatic lens based on a signal indicative of a distance of a surface of a substrate from a portion of the first magnetic lens disposed closest to the substrate.

Abstract: A charged particle system comprises a particle source for generating a beam of charged particles and a particle-optical projection system. The particle-optical projection system comprises a focusing first magnetic lens (403) comprising an outer pole piece (411) having a radial inner end (411?), and an inner pole piece (412) having a lowermost end (412?) disposed closest to the radial inner end of the outer pole piece, a gap being formed by those; a focusing electrostatic lens (450) having at least a first electrode (451) and a second electrode (450) disposed in a region of the gap; and a controller (C) configured to control a focusing power of the first electrostatic lens based on a signal indicative of a distance of a surface of a substrate from a portion of the first magnetic lens disposed closest to the substrate.

Abstract: In a particle multibeam lithography apparatus an illumination system (242) having a particle source (203) produces an illuminating beam (205) of electrically charged particles, and a multibeam optical system (208) positioned after the illumination system (242) and comprising at least one aperture plate having an array of a plurality of apertures to form a plurality of sub-beams focuses the sub-beams onto the surface of a substrate (220), wherein for each sub-beam (207) a deflection unit (210) is positioned within the multibeam optical system and adapted to correct individual imaging aberrations of the respective sub-beam with respect to the desired target position and/or position the sub-beam during a writing process an the substrate surface.

Abstract: A device (102) for defining a pattern, for use in a particle-beam exposure apparatus (100), said device adapted to be irradiated with a beam (lb,pb) of electrically charged particles and let pass the beam only through a plurality of apertures, comprises an aperture array means (203) and a blanking means (202). The aperture array means (203) has a plurality of apertures (21,230) of identical shape defining the shape of beamlets (bm). The blanking means (202) serves to switch off the passage of selected beamlets; it has a plurality of openings (220), each corresponding to a respective aperture (230) of the aperture array means (203) and being provided with a deflection means (221) controllable to deflect particles radiated through the opening off their path (p1) to an absorbing surface within said exposure apparatus (100). The apertures (21) are arranged on the blanking and aperture array means (202,203) within a pattern definition field (pf) being composed of a plurality of staggered lines (p1) of apertures.

Abstract: In a particle multibeam lithography apparatus an illumination system (242) having a particle source (203) produces an illuminating beam (205) of electrically charged particles, and a multibeam optical system (208) positioned after the illumination system (242) and comprising at least one aperture plate having an array of a plurality of apertures to form a plurality of sub-beams focuses the sub-beams onto the surface of a substrate (220), wherein for each sub-beam (207) a deflection unit (210) is positioned within the multibeam optical system and adapted to correct individual imaging aberrations of the respective sub-beam with respect to the desired target position and/or position the sub-beam during a writing process an the substrate surface Preferably, for each sub-beam the respective aperture of the first aperture plate defines the size and shape of the sub-beam cross-section and the multibeam optical system produces a demagnified image of the aperture on the substrate surface, with a demagnification of at

Abstract: A device (102) for defining a pattern, for use in a particle-beam exposure apparatus (100), said device adapted to be irradiated with a beam (lb,pb) of electrically charged particles and let pass the beam only through a plurality of apertures, comprises an aperture array means (203) and a blanking means (202). The aperture array means (203) has a plurality of apertures (21,230) of identical shape defining the shape of beamlets (bm). The blanking means (202) serves to switch off the passage of selected beamlets; it has a plurality of openings (220), each corresponding to a respective aperture (230) of the aperture array means (203) and being provided with a deflection means (221) controllable to deflect particles radiated through the opening off their path (p1) to an absorbing surface within said exposure apparatus (100). The apertures (21) are arranged on the blanking and aperture array means (202,203) within a pattern definition field (pf) being composed of a plurality of staggered lines (p1) of apertures.

Abstract: A process is disclosed for producing a structured mask for use in reproducing structures of that mask on an object with the aid of electromagnetic or particulate radiation, in particular for ion beam lithography. A flat smooth substrate of more than 20 .mu.m in thickness is selected and a thin diaphragm is produced from that substrate by etching one of the sections removed from the edging to a depth of c. 0.5-20 .mu.m, the tensile stress within the diaphragm being greater than 5 MPa. Lithographic structures are then formed on a central region of the diaphragm with a tensile stress of more than 5 MPa; apertures are etched into the diaphragm to form the mask structures and the effective thickness inside a diaphragm region substantially enclosing the mask structures is reduced, causing the central region containing the structures to be joined to the substrate edging elastically in such a way that the mean tensile stress within this central region is reduced to below 5 MPa.

Abstract: An arrangement for shadow-casting lithography by focusing electrically charged particles for the purpose of imaging structures of a mask on a substrate disposed immediately to the rear thereof, comprising a particle source (2) and an extraction system (3) which produces a divergent particle beam issuing from a substantially point-shaped virtual source, and comprising a lens (6) for focusing the divergent particle beam which comprises an electrode arrangement (6a, 6b, 6c, 6d, 6e, 6f, 6g, 6h) which includes at least one electrostatic collector lens (6a to 6f in conjunction with an electrostatic diverging lens (6g, 6h) in order to be able to compensate lens errors of the collector lens in a purposeful manner with respect to lens errors of the diverging lens and to render possible a predeterminable change in the imaging scale.

Abstract: A particle beam, in particular in ionic on the reproduction system, preferably for lithographic purposes, has a particle source, in particular an ion source for reproducing on a wafer a structure designed in a masking foil as one or several transparent spots, in particular openings, through at least two electrostatic lenses arranged upstream of the wafer. One of the lenses is a grating lens constituted by one or two tubular electrodes and by a perforated plate arranged in the path of the beam perpendicularly to the optical axis. The plate is formed by a masking foil which forms the central or first electrode of the granting lens, in the direction of propagation of the beam.

Abstract: An arrangement for masked beam lithography by means of electrically charged particles for the imaging of structures of a mask on a substrate arranged behind it, with a substantially punctiform particle source (Q) and an extraction system (Ex) for a specific type of charged particles which leave the source (Q) in the form of a divergent particle beam, and with an electrode arrangement (B, B', El.sub.1, El.sub.2, E.sub.3, . . . El.sub.n) for concentrating the divergent particle beam into a particle beam which is at least approximately parallel, by means of which an electrostatic acceleration field (E) is generated, the potential (U) of which in the beam direction has a constant gradient at least in parts and perpendicular to the beam direction is substantially constant at least within the beam cross-section. The electrode arrangement can be formed for example by a plurality of coaxial ring electrodes (El.sub.1, El.sub.2, El.sub.3, . . . El.sub.

Abstract: A charged particle, in particular ion projector system, has a mask arranged in the path of the charged particle beam and provided with transparent spots, in particular openings, arranged asymmetrically to the optical axis, which are reproduced on a wafer by means of lenses arranged in the path of the charged particle beam. The charged particle beam has at least one cross-over (crosses the optical axis at least once) between the mask and the wafer. Charged particles with an opposite charge to the charge of the reproduction particles are supplied into the path of the reproduction charged particle beam in a defined area located between the mask and the wafer. The limits that define said area are selected in such a way that the absolute value of the integral effect of the space charge on the particles that reproduce the mask structures is as high upstream of said area (seen in the direction of radiation) as the absolute value of the integral effect of the space charge downstream of said area.

Abstract: A system for ion-beam imaging of a structure of a mask on a wafer has a two-lens set between the mask and the wafer which is made up of a preferably accelerating Einzel lens proximal to the mask and an asymmetric accelerating Einzel proximal to the wafer.

Abstract: In an ion optical imaging system, especially for lithographic imaging on a wafer, two collecting lenses are provided between the mask and the wafer. At least one of the collecting lenses is a three-electrode grid lens, i.e. a lens in which a grid is disposed perpendicular to the optical axis between a pair of tubular electrodes.