A particle beam system includes a multiple beam particle source to generate a multiplicity of charged individual particle beams, and a multi-pole lens sequence with first and second multi-pole lens arrays. The particle beam system also includes a controller to control the multi-pole lenses of the multi-pole lens sequence so related groups of multi-pole lenses of the multi-pole lens sequence through which the same individual particle beam passes in each case altogether exert an individually adjustable and focussing effect on the respective individual particle beam passing therethrough.

An objective lens arrangement includes a first, second and third pole pieces, each being substantially rotationally symmetric. The first, second and third pole pieces are disposed on a same side of an object plane. An end of the first pole piece is separated from an end of the second pole piece to form a first gap, and an end of the third pole piece is separated from an end of the second pole piece to form a second gap. A first excitation coil generates a focusing magnetic field in the first gap, and a second excitation coil generates a compensating magnetic field in the second gap. First and second power supplies supply current to the first and second excitation coils, respectively. A magnetic flux generated in the second pole piece is oriented in a same direction as a magnetic flux generated in the second pole piece.

An objective lens arrangement includes a first, second and third pole pieces, each being substantially rotationally symmetric. The first, second and third pole pieces are disposed on a same side of an object plane. An end of the first pole piece is separated from an end of the second pole piece to form a first gap, and an end of the third pole piece is separated from an end of the second pole piece to form a second gap. A first excitation coil generates a focusing magnetic field in the first gap, and a second excitation coil generates a compensating magnetic field in the second gap. First and second power supplies supply current to the first and second excitation coils, respectively. A magnetic flux generated in the second pole piece is oriented in a same direction as a magnetic flux generated in the second pole piece.

A multi-charged particle beam writing apparatus according to one aspect of the present invention includes a region setting unit configured to set, as an irradiation region for a beam array to be used, the region of the central portion of an irradiation region for all of multiple beams of charged particle beams implemented to be emittable by a multiple beam irradiation mechanism, and a writing mechanism, including the multiple beam irradiation mechanism, configured to write a pattern on a target object with the beam array in the region of the central portion having been set in the multiple beams implemented.

A multi-charged particle beam writing apparatus according to one aspect of the present invention includes a region setting unit configured to set, as an irradiation region for a beam array to be used, the region of the central portion of an irradiation region for all of multiple beams of charged particle beams implemented to be emittable by a multiple beam irradiation mechanism, and a writing mechanism, including the multiple beam irradiation mechanism, configured to write a pattern on a target object with the beam array in the region of the central portion having been set in the multiple beams implemented.

The present invention relates to a monochromator device. The monochromator device includes a first radiofrequency cavity positioned to receive an output beam from an electron source. A second radiofrequency cavity is positioned to receive the output beam from the first radiofrequency cavity. The first radiofrequency cavity and the second radiofrequency cavity are configured to, in combination, in combination, correct one or more energy deviations in time and space of the output beam.

The present invention relates to a monochromator device. The monochromator device includes a first radiofrequency cavity positioned to receive an output beam from an electron source. A second radiofrequency cavity is positioned to receive the output beam from the first radiofrequency cavity. The first radiofrequency cavity and the second radiofrequency cavity are configured to, in combination, in combination, correct one or more energy deviations in time and space of the output beam.

To provide a charged particle beam device including a booster electrode and an object lens that generates a magnetic field in a vicinity of a sample, and capable of preventing ion discharge, an insulator is disposed between a magnetic field lens and the booster electrode. A tip of the insulator protrudes to a tip side of an upper magnetic path from a tip of a lower magnetic path of the magnetic field lens. The tip on a lower side of the insulator is above the lower magnetic path, and a non-magnetic metal electrode is embedded between the upper magnetic path and the lower magnetic path.

A multi-electron beam image acquisition apparatus includes: a first electromagnetic lens configured to focus the multiple primary electron beams to form an image on the substrate; and a second electromagnetic lens configured to be able to variably adjust a peak position of a magnetic field distribution in a direction of a trajectory central axis of the multiple secondary electron beams, and to focus the multiple secondary electron beams to form an image on either one of a detection surface of the detector and a position conjugate to the detection surface, wherein the first electromagnetic lens focuses, to form an image, the multiple secondary electron beams in a state before being separated from the multiple primary electron beams, and the second electromagnetic lens is arranged between the separator and an image forming point on which the multiple secondary electron beams are focused by the first electromagnetic lens.

A multi-electron beam image acquisition apparatus includes: a first electromagnetic lens configured to focus the multiple primary electron beams to form an image on the substrate; and a second electromagnetic lens configured to be able to variably adjust a peak position of a magnetic field distribution in a direction of a trajectory central axis of the multiple secondary electron beams, and to focus the multiple secondary electron beams to form an image on either one of a detection surface of the detector and a position conjugate to the detection surface, wherein the first electromagnetic lens focuses, to form an image, the multiple secondary electron beams in a state before being separated from the multiple primary electron beams, and the second electromagnetic lens is arranged between the separator and an image forming point on which the multiple secondary electron beams are focused by the first electromagnetic lens.