A charged particle beam writing method includes forming an aperture image by making a charged particle beam pass through an aperture substrate, changing, in the state where a plurality of crossover positions of the charged particle beam and positions of all of one or more intermediate images of the aperture image are adjusted to matching positions with respect to the aperture image with the first magnification, magnification of the aperture image from the first magnification to the second magnification by using a plurality of lenses while maintaining the last crossover position of the charged particle beam and the position of the last intermediate image of the aperture image to be fixed, and forming, using an objective lens, the aperture image whose magnification has been changed to the second magnification on the surface of the target object, and writing the aperture image.

A multi-beam apparatus for observing a sample with high resolution and high throughput is proposed. In the apparatus, a source-conversion unit changes a single electron source into a virtual multi-source array, a primary projection imaging system projects the array to form plural probe spots on the sample, and a condenser lens adjusts the currents of the plural probe spots. In the source-conversion unit, the image-forming means is on the upstream of the beamlet-limit means, and thereby generating less scattered electrons. The image-forming means not only forms the virtual multi-source array, but also compensates the off-axis aberrations of the plurality of probe spots.

A multi-beam apparatus for observing a sample with high resolution and high throughput is proposed. In the apparatus, a source-conversion unit changes a single electron source into a virtual multi-source array, a primary projection imaging system projects the array to form plural probe spots on the sample, and a condenser lens adjusts the currents of the plural probe spots. In the source-conversion unit, the image-forming means is on the upstream of the beamlet-limit means, and thereby generating less scattered electrons. The image-forming means not only forms the virtual multi-source array, but also compensates the off-axis aberrations of the plurality of probe spots.

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.

An ion implantation apparatus includes: a multistage linear acceleration unit including a plurality of stages of high-frequency resonators and a plurality of stages of focusing lenses; a first beam measuring unit disposed in the middle of the multistage linear acceleration unit and configured to allow passage of a beam portion adjacent to a center of a beam trajectory and measure a current intensity of another beam portion blocked by an electrode body outside a vicinity of the center of the beam trajectory; a second beam measuring unit disposed downstream of the multistage linear acceleration unit and configured to measure a current intensity of an ion beam exiting from the multistage linear acceleration unit; and a control device configured to adjust a control parameter of the plurality of stages of focusing lenses based on measurement results of the first and second beam measuring units.

Provided herein are approaches for controlling a charged particle beam using a series of electrodes including a plurality of different shapes. In one approach, an electrostatic optical element includes a first set of electrodes having a first electrode shape for parallelizing and deflecting the charged particle beam using a first set of electrodes having a first electrode shape, such as a concave or convex profile. The electrostatic optical element further includes a second set of electrodes adjacent the first set of electrodes for accelerating or decelerating the charged particle beam along a beamline, wherein the second set of electrodes include a cylindrical shape. In one approach, a power supply is electrically connected to the first and second sets of electrodes, the power supply arranged to enable independent voltage/current control.

A method of imaging an object in a first material having a different charge density to the object is provided, the method comprising: focusing a charged particle beam to a virtual charged particle beam source in the first material; moving the virtual charged particle beam source in and around the object to provide at least one charged particle reflected object beam or at least one charged particle refracted object beam and at least one charged particle bypass beam, wherein the charged particle reflected object beam or the charged particle refracted object beam and the charged particle bypass beam intercept one another to form an interference zone; and defocusing the interference zone to provide a Fresnel fringe, the Fresnel fringe forming an image of the object; or focusing the virtual charged particle beam source on the object to provide a first lower energy charged particle beam and a second lower energy charged particle beam, wherein the first lower energy charged particle beam and the second lower energy charged particle beam intercept one another to form a self-interference zone; defocusing the self-interference zone to provide a Fresnel fringe, the Fresnel fringe forming an image of the object.

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.

An electrostatic lens comprising a first conductive plate with a first aperture, a second conductive plate with a second aperture, the second aperture being substantially aligned with the first aperture, a voltage supply for supplying a first voltage to the first conductive plate and a second voltage to the second conductive plate, the first voltage being lower than the second voltage, and an insulating structure for separating the first conductive plate from the second conductive plate. The insulating structure comprises a first portion in contact with the first conductive plate and a second portion in contact with the second conductive plate, the first portion having an overhanging portion and the second portion having an indented portion at an edge of the insulating structure, so that a gap is formed between the overhanging portion and the second conductive plate.

A multi-beam apparatus for observing a sample with high resolution and high throughput is proposed. In the apparatus, a source-conversion unit changes a single electron source into a virtual multi-source array, a primary projection imaging system projects the array to form plural probe spots on the sample, and a condenser lens adjusts the currents of the plural probe spots. In the source-conversion unit, the image-forming means is on the upstream of the beamlet-limit means, and thereby generating less scattered electrons. The image-forming means not only forms the virtual multi-source array, but also compensates the off-axis aberrations of the plurality of probe spots.