The disclosure relates to an electron-optical module of an electron-optical apparatus. The electron-optical module comprises a vacuum chamber, a high voltage shielding arrangement located within the vacuum chamber, and an aperture array configured to form a plurality of beamlets from an electron beam and located within the high voltage shielding arrangement. Wherein the electron-optical module can be configured to be removable from the electron-optical apparatus.

The disclosure relates to an electron-optical module of an electron-optical apparatus. The electron-optical module comprises a vacuum chamber, a high voltage shielding arrangement located within the vacuum chamber, and an aperture array configured to form a plurality of beamlets from an electron beam and located within the high voltage shielding arrangement. Wherein the electron-optical module can be configured to be removable from the electron-optical apparatus.

A flood column for charged particle flooding of a sample, the flood column comprising a charged particle source configured to emit a charged particle beam along a beam path; a source lens arranged down-beam of the charged particle source; a condenser lens arranged down-beam of the source lens; and an aperture body arranged down-beam of the condenser lens, wherein the aperture body is for passing a portion of the charged particle beam; and wherein the source lens is controllable so as to variably set the beam angle of the charged particle beam down-beam of the source lens.

A flood column for charged particle flooding of a sample, the flood column comprising a charged particle source configured to emit a charged particle beam along a beam path; a source lens arranged down-beam of the charged particle source; a condenser lens arranged down-beam of the source lens; and an aperture body arranged down-beam of the condenser lens, wherein the aperture body is for passing a portion of the charged particle beam; and wherein the source lens is controllable so as to variably set the beam angle of the charged particle beam down-beam of the source lens.

A charged particle system generates a charged particle multi beam along a multi beam path. The charged particle system comprises an aperture array, a beam limit array and a condenser lens. In the aperture array are an array of apertures to generate from an up-beam charged particle source charged particle paths down-beam of the aperture array. The beam-limit array is down-beam of the aperture array. Defined in the beam-limit array is an array of beam-limit apertures for shaping the charged particle multi beam path. The condenser lens system is between the aperture array and the beam-limit array. The condenser lens system selectively operates different of rotation settings that define different ranges of beam paths between the aperture array and the beam-limit array. At each rotation setting of the condenser lens system, each beam-limit aperture of the beam-limit array lies on a beam path down-beam of the aperture array.

A charged particle system generates a charged particle multi beam along a multi beam path. The charged particle system comprises an aperture array, a beam limit array and a condenser lens. In the aperture array are an array of apertures to generate from an up-beam charged particle source charged particle paths down-beam of the aperture array. The beam-limit array is down-beam of the aperture array. Defined in the beam-limit array is an array of beam-limit apertures for shaping the charged particle multi beam path. The condenser lens system is between the aperture array and the beam-limit array. The condenser lens system selectively operates different of rotation settings that define different ranges of beam paths between the aperture array and the beam-limit array. At each rotation setting of the condenser lens system, each beam-limit aperture of the beam-limit array lies on a beam path down-beam of the aperture array.

A Schottky thermal field emitter (TFE) source integrated with a beam splitter by a standoff, which supports the beam splitter above the Schottky TFE extractor faceplate by a distance of 0.05 mm to 2 mm. The beam splitter includes a microhole array integrated with the standoff and being disposed opposite the extractor faceplate, the microhole array having a plurality of microholes that split the electron beam generated by the Schottky TFE into a plurality of beamlets. The support and extractor may be fabricated from the same material or from different materials. The support may be formed from a high temperature resistive material, which causes a potential difference between the extractor and the microhole array. This potential difference creates positively charged electrostatic lenses at the microholes, which increases current in the individual beamlets. Voltage on the microarray plate may be varied to achieve a high beamlet current.

A Schottky thermal field emitter (TFE) source integrated with a beam splitter by a standoff, which supports the beam splitter above the Schottky TFE extractor faceplate by a distance of 0.05 mm to 2 mm. The beam splitter includes a microhole array integrated with the standoff and being disposed opposite the extractor faceplate, the microhole array having a plurality of microholes that split the electron beam generated by the Schottky TFE into a plurality of beamlets. The support and extractor may be fabricated from the same material or from different materials. The support may be formed from a high temperature resistive material, which causes a potential difference between the extractor and the microhole array. This potential difference creates positively charged electrostatic lenses at the microholes, which increases current in the individual beamlets. Voltage on the microarray plate may be varied to achieve a high beamlet current.

An electrostatic device includes a top and a bottom silicon layer, around an insulating buried layer. A beam opening allows a beam of charged particles to travel through. The device is encapsulated in an insulating layer. One or more electrodes and ground planes are deposited on the insulating layer. These also cover the inside of the beam opening. Electrodes and ground planes are physically and electrically separated by micro-trenches and micro-undercuts that provide shadow areas when the conductive areas are deposited. Electrodes may be shaped as elongated islands and may include portions overhanging the top silicon layer, supported by electrode-anchors. Manufacturing starts from a single wafer including the top, buried, and bottom layers, or it starts from two separate silicon wafers. Manufacturing includes steps to form the top and bottom beam openings and microstructures, to encapsulate the device in an insulating layer, and to deposit electrodes and ground areas.

An electrostatic device includes a top and a bottom silicon layer, around an insulating buried layer. A beam opening allows a beam of charged particles to travel through. The device is encapsulated in an insulating layer. One or more electrodes and ground planes are deposited on the insulating layer. These also cover the inside of the beam opening. Electrodes and ground planes are physically and electrically separated by micro-trenches and micro-undercuts that provide shadow areas when the conductive areas are deposited. Electrodes may be shaped as elongated islands and may include portions overhanging the top silicon layer, supported by electrode-anchors. Manufacturing starts from a single wafer including the top, buried, and bottom layers, or it starts from two separate silicon wafers. Manufacturing includes steps to form the top and bottom beam openings and microstructures, to encapsulate the device in an insulating layer, and to deposit electrodes and ground areas.