A method for calibrating a scanning charged particle microscope, such as a scanning electron microscope (SEM), is provided. The method includes dividing a wafer into a plurality of regions; preparing, on each of the plurality of regions, a pattern including a first periodic structure interleaved with a second periodic structure, the first and second periodic structures having an induced offset; determining an actual pitch the first and second periodic structures and thereby determining actual induced offset on each of the plurality of regions; selecting a plurality of regions from among the plurality of regions; measuring, by the SEM, a pitch of first and second periodic structures on each of the plurality of regions; and performing linearity calibration on the SEM based on the determining and the measuring.

An ion implantation system and method provide a non-uniform flux of a ribbon ion beam. A spot ion beam is formed and provided to a scanner, and a scan waveform having a time-varying potential is applied to the scanner. The ion beam is scanned by the scanner across a scan path, generally defining a scanned ion beam comprised of a plurality of beamlets. The scanned beam is then passed through a corrector apparatus. The corrector apparatus is configured to direct the scanned ion beam toward a workpiece at a generally constant angle of incidence across the workpiece. The corrector apparatus further comprises a plurality of magnetic poles configured to provide a non-uniform flux profile of the scanned ion beam at the workpiece.

A multi-beam apparatus for observing a sample with high resolution and high throughput is proposed. In the apparatus, a source-conversion unit forms plural and parallel images of one single electron source by deflecting plural beamlets of a parallel primary-electron beam therefrom, and one objective lens focuses the plural deflected beamlets onto a sample surface and forms plural probe spots thereon. A movable condenser lens is used to collimate the primary-electron beam and vary the currents of the plural probe spots, a pre-beamlet-forming means weakens the Coulomb effect of the primary-electron beam, and the source-conversion unit minimizes the sizes of the plural probe spots by minimizing and compensating the off-axis aberrations of the objective lens and condenser lens.

A charged particle beam device that detects a secondary charged particle beam generated by irradiation of a sample by a primary charged particle beam, includes: an image shift deflector that shifts an irradiation region for irradiation of the sample by the primary charged particle beam; a magnetic sector that separates the primary charged particle beam passing therein from the secondary charged particle beam from the sample using a magnetic field generated therein; a correction mechanism that is placed off of a trajectory of the primary charged particle beam but on a trajectory of the secondary charged particle beam inside the magnetic sector, the correction mechanism deflecting the secondary charged particle beam passing through; and a controller that controls the correction mechanism according to a defined relationship between a shift amount by the image shift deflector and a correction amount by the correction mechanism.

An object of the invention is to correct an aberration or a defocus of an electron beam for irradiation, and control an influence on a deflector by a fluctuation in an electric field of an electrostatic lens. The invention provides a charged particle beam apparatus including a deflector that deflects a charged particle beam with which a specimen is irradiated, an objective lens that focuses the charged particle beam on the specimen, an electrostatic lens that includes a part of the objective lens and to which a voltage for correcting the aberration or the defocus of the charged particle beam is applied, and an constant electric field applying electrode that is provided between the deflector and the electrostatic lens and to which a constant voltage having a same sign with the voltage applied to the electrostatic lens is applied.

A multiple charged particle beam writing apparatus includes a rotatable shaping aperture array substrate, including plural openings, to form/shape multiple beams by letting portions of a charged particle beam individually pass through the plural openings, a data rotation correction circuitry to read writing data from a storage device, and generate pattern data, in which the entire figure pattern has been reversely rotated against a rotational deviation direction of an aperture array image by a rotational deviation amount of the aperture array image, using information on the rotational deviation amount of the aperture array image of the multiple beams on the target object caused by a residual error of rotation adjustment of the shaping aperture array substrate, and a blanking aperture array mechanism, rotatable with the shaping aperture array substrate, to provide individual blanking control of the multiple beams, based on the pattern data of the figure pattern reversely rotated.

An ion implantation system and method provide a non-uniform flux of a ribbon ion beam. A spot ion beam is formed and provided to a scanner, and a scan waveform having a time-varying potential is applied to the scanner. The ion beam is scanned by the scanner across a scan path, generally defining a scanned ion beam comprised of a plurality of beamlets. The scanned beam is then passed through a corrector apparatus. The corrector apparatus is configured to direct the scanned ion beam toward a workpiece at a generally constant angle of incidence across the workpiece. The corrector apparatus further comprises a plurality of magnetic poles configured to provide a non-uniform flux profile of the scanned ion beam at the workpiece.

A charged particle beam device includes an electron source which generates an electron beam, an objective lens which is applied with a coil current to converge the electron beam on a sample, a control unit which controls the current to be applied to the objective lens, a hysteresis characteristic storage unit which stores hysteresis characteristic information of the objective lens, a history information storage unit which stores history information related to the coil current, and an estimation unit which estimates a magnetic field generated by the objective lens on the basis of the coil current, the history information, and the hysteresis characteristic information.

A distortion measurement method for an electron microscope image includes: loading a distortion measurement specimen having structures arranged in a lattice to a specimen plane of an electron microscope or a plane conjugate to the specimen plane in order to obtain an electron microscope image of the distortion measurement specimen; and measuring a distortion from the obtained electron microscope image of the distortion measurement specimen.

A multi-beam apparatus for observing a sample with high resolution and high throughput is proposed. In the apparatus, a source-conversion unit forms plural and parallel images of one single electron source by deflecting plural beamlets of a parallel primary-electron beam therefrom, and one objective lens focuses the plural deflected beamlets onto a sample surface and forms plural probe spots thereon. A movable condenser lens is used to collimate the primary-electron beam and vary the currents of the plural probe spots, a pre-beamlet-forming means weakens the Coulomb effect of the primary-electron beam, and the source-conversion unit minimizes the sizes of the plural probe spots by minimizing and compensating the off-axis aberrations of the objective lens and condenser lens.