A multi-beam pattern definition device for use in a particle-beam processing or inspection apparatus, which is irradiated with a beam of electrically charged particles and allows passage of the beam through a plurality of apertures to form corresponding beamlets, comprises an aperture array device in which said apertures are realized according to several sets of apertures arranged in respective aperture arrangements, and an absorber array device having a plurality of openings configured for the passage of at least a subset of beamlets that are formed by the apertures. The absorber array device comprises a plurality of openings corresponding to one of the aperture arrangements of the aperture array device, whereas it includes a charged-particle absorbing structure comprising absorbing regions surrounded by elevated regions and configured to absorb charged particles impinging thereupon at locations corresponding to apertures of the other aperture arrangements of the aperture array device, effectively confining the effects of irradiated particles and electric charge therein.

Lithographic apparatuses suitable for complementary e-beam lithography (CEBL) are described. In an example, a method of forming a pattern for a semiconductor structure includes forming a pattern of parallel lines above a substrate. The method also includes aligning the substrate in an e-beam tool to provide the pattern of parallel lines parallel with a scan direction of the e-beam tool. The e-beam tool includes a column having a blanker aperture array (BAA) with a staggered pair of columns of openings along an array direction orthogonal to the scan direction. The method also includes forming a pattern of cuts or vias in or above the pattern of parallel lines to provide line breaks for the pattern of parallel lines by scanning the substrate along the scan direction. A cumulative current through the column has a non-zero and substantially uniform cumulative current value throughout the scanning.

Provided is a charged particle beam device with low blanking noise and improved signal detection accuracy. As means therefor, a charged particle beam device is configured by: a stage where a sample is mountable; a charged particle gun performing charged particle emission to the sample; a voltage source; a first switching circuit to which a voltage is supplied from the voltage source; a second switching circuit having one end connected to a ground; a third switching circuit having one end connected to the ground; a fourth switching circuit to which a voltage is supplied from the voltage source; a first blanking electrode connected to the first switching circuit and the second switching circuit; a second blanking electrode facing the first blanking electrode and connected to the third switching circuit and the fourth switching circuit; and a control circuit controlling the first switching circuit, the second switching circuit, the third switching circuit, and the fourth switching circuit.

Electron beam modulation in response to optical pump pulses applied to a sample is measured using SPAD elements. Individual detection events are used to form histograms of numbers of events in time bins associated with pump pulse timing. The histograms can be produced at a SPAD array, simplifying data transfer. In some examples, two SPAD arrays are stacked and a coincidence circuit discriminates signal events from noise events by determining corresponding events are detected within a predetermined time window.

Systems and methods for reducing the buildup of charge during the investigation of samples using charged particle beams, according to the present disclosure include irradiating a first portion of a sample during a first time period, wherein the irradiating the first portion of the sample causes a gradual accumulation of net charge in the first portion of the sample, generating imaging data based on emissions resultant from irradiating the first portion of the sample, and then irradiating a second portion of a sample holder for a second time period. The methods may further includes iteratively repeating the irradiation of the first portion and the second portion during imaging of the sample region. When more than one region of interest on the sample is to be investigated, the method may also include continuing to image additional portions of the sample by iteratively irradiating a region of interest on the sample and a corresponding portion of the sample holder.

Disclosed herein is an aperture body for passing a portion of a charged particle beam propagating along a beam path comprising an axis, the aperture body comprising: an up-beam facing surface; a chamber portion comprising an up-beam end, a down-beam end and an up-beam plate, wherein the up-beam plate extends radially inwards from the up-beam end and the up-beam plate is configured to define an entrance opening around the beam path; wherein: the up-beam facing surface extends radially inwards from the down-beam end; the up-beam facing surface comprises an aperture portion that is configured to define an opening around the beam path; and the opening defined by the aperture portion is smaller than the entrance opening.

The present invention quickly calculates values of optimal excitation parameters which are set in lenses in multiple stages. A multi charged particle beam adjustment method includes forming a multi charged particle beam, calculating, for each of lenses in two or more stages disposed corresponding to object lenses in two or more stages, a first rate of change and a second rate of change in response to change in at least an excitation parameter, the first rate of change being a rate of change in a demagnification level of a beam image of the multi charged particle beam, the second rate of change being a rate of change in a rotation level of the beam image, and calculating a first amount of correction to the excitation parameter of each of the lenses based on an amount of correction to the demagnification level and the rotation level of the beam image, the first rate of change, and the second rate of change.

Systems and methods for reducing the buildup of charge during the investigation of samples using charged particle beams, according to the present disclosure include irradiating a first portion of a sample during a first time period, wherein the irradiating the first portion of the sample causes a gradual accumulation of net charge in the first portion of the sample, generating imaging data based on emissions resultant from irradiating the first portion of the sample, and then irradiating a second portion of a sample holder for a second time period. The methods may further includes iteratively repeating the irradiation of the first portion and the second portion during imaging of the sample region. When more than one region of interest on the sample is to be investigated, the method may also include continuing to image additional portions of the sample by iteratively irradiating a region of interest on the sample and a corresponding portion of the sample holder.

Apparatuses, systems, and methods for multi-modal operations of a multi-beam inspection system are disclosed. An apparatus for generating multi-modal beamlets may include an aperture array which includes a first group of apertures having a first size and a second group of apertures having a second size different from the first size, the second group of apertures adjoining the first group of apertures, in which the first group of apertures and the second group of apertures are in different pass-or-block statuses. A multi-beam apparatus of multi-modal inspection operations may include the aforementioned apparatus, a source configured to emit charged particles, a condenser system configured to set a projection area of the charged particles, and circuitry for controlling the first and second groups of apertures.

Electron beam modulation in response to optical pump pulses applied to a sample is measured using SPAD elements. Individual detection events are used to form histograms of numbers of events in time bins associated with pump pulse timing. The histograms can be produced at a SPAD array, simplifying data transfer. In some examples, two SPAD arrays are stacked and a coincidence circuit discriminates signal events from noise events by determining corresponding events are detected withing a predetermined time window.