A multi-beam apparatus for observing a sample with high resolution and high throughput and in flexibly varying observing conditions is proposed. The apparatus uses a movable collimating lens to flexibly vary the currents of the plural probe spots without influencing the intervals thereof, a new source-conversion unit to form the plural images of the single electron source and compensate off-axis aberrations of the plural probe spots with respect to observing conditions, and a pre-beamlet-forming means to reduce the strong Coulomb effect due to the primary-electron beam.

A collimated electron beam is illuminated to a grounded metal mask such that patterns on the mask can be transferred to a substrate identically. In a preferred embodiment, a linear electron source can be provided for enhancing lithographic throughput. The metal mask is adjacent to the substrate, but does not contact with substrate.

A multi-beam apparatus for observing a sample with high resolution and high throughput and in flexibly varying observing conditions is proposed. The apparatus uses a movable collimating lens to flexibly vary the currents of the plural probe spots without influencing the intervals thereof, a new source-conversion unit to form the plural images of the single electron source and compensate off-axis aberrations of the plural probe spots with respect to observing conditions, and a pre-beamlet-forming means to reduce the strong Coulomb effect due to the primary-electron beam.

A multi-beam electron source is disclosed. The multi-beam source includes an electron source, a grid lens assembly, and a multi-lens array assembly. The multi-lens array assembly includes a set of lenses disposed across a substrate. The grid lens assembly is configured to cause a primary electron beam from the electron beam source to land on the multi-lens array assembly telecentrically. The multi-lens array assembly is configured to split the electron beam from the electron beam source into a plurality of primary electron beams. The grid lens assembly includes a first lens element and a second lens element, wherein the first lens element and the second lens element are separated by a gap of a selected distance. The grid lens assembly further includes a grid element including a set of apertures, wherein the grid element is disposed within the gap between the first lens element and the second lens element.

Situating samples on an optical axis of a charged particle microscope can be performed based a 3D map of the samples. The 3D map is produced with back-side illumination of the samples and telecentric imaging to produce profile images. The profile images are a combined to form the 3D map. Using the 3D map, the processor is coupled to a sample stage to situate a selected sample or sample portion for imaging in the charged particle microscope. In some examples, the processor is responsive to selection of a sample using a graphical interface so that the sample stage is controlled to safely situate the selected sample without further operator intervention.

A method includes operating a multiple particle beam system at different working points. The numerical aperture can be set for each of the working points in such a way that the resolution of the multiple particle beam system is optimal. In the process, the beam pitch between adjacent individual particle beams on the sample to be scanned is kept constant as a boundary condition. There are no mechanical reconfigurations of the system whatsoever for the purposes of varying the numerical aperture.

A particle beam system and, such as a multi-beam particle microscope, can have a current intensity of individual particle beams that is flexibly set over large value ranges without structural modifications. The particle beam system can include a condenser lens system, a pre-multi-lens array with a specific pre-counter electrode and a pre-multi-aperture plate, and a multi-lens array. The system can includes a controller to supply adjustable excitations to the condenser lens system and the pre-counter electrode so that the charged particles are incident on the pre-multi-aperture plate in telecentric manner.

Situating samples on an optical axis of a charged particle microscope can be performed based a 3D map of the samples. The 3D map is produced with back-side illumination of the samples and telecentric imaging to produce profile images. The profile images are a combined to form the 3D map. Using the 3D map, the processor is coupled to a sample stage to situate a selected sample or sample portion for imaging in the charged particle microscope. In some examples, the processor is responsive to selection of a sample using a graphical interface so that the sample stage is controlled to safely situate the selected sample without further operator intervention.

A multi-beam apparatus for observing a sample with high resolution and high throughput and in flexibly varying observing conditions is proposed. The apparatus uses a movable collimating lens to flexibly vary the currents of the plural probe spots without influencing the intervals thereof, a new source-conversion unit to form the plural images of the single electron source and compensate off-axis aberrations of the plural probe spots with respect to observing conditions, and a pre-beamlet-forming means to reduce the strong Coulomb effect due to the primary-electron beam.

A multi-beam apparatus for observing a sample with high resolution and high throughput and in flexibly varying observing conditions is proposed. The apparatus uses a movable collimating lens to flexibly vary the currents of the plural probe spots without influencing the intervals thereof, a new source-conversion unit to form the plural images of the single electron source and compensate off-axis aberrations of the plural probe spots with respect to observing conditions, and a pre-beamlet-forming means to reduce the strong Coulomb effect due to the primary-electron beam.