Electron gun systems with a particular inner width dimension, sweep electrodes, or a combination of a particular inner width dimension and sweep electrodes are disclosed. The inner width dimension may be less than twice a value of a Larmor radius of secondary electrons in a channel downstream of a beam limiting aperture, and a Larmor time for the secondary electrons may be greater than 1 ns. The sweep electrode can generates an electric field in a drift region, which can increase kinetic energy of secondary electrons in the channel.

Electron gun systems with a particular inner width dimension, sweep electrodes, or a combination of a particular inner width dimension and sweep electrodes are disclosed. The inner width dimension may be less than twice a value of a Larmor radius of secondary electrons in a channel downstream of a beam limiting aperture, and a Larmor time for the secondary electrons may be greater than 1 ns. The sweep electrode can generates an electric field in a drift region, which can increase kinetic energy of secondary electrons in the channel.

An electron source is disclosed. The electron source may include an electron emitter configured to generate one or more electron beams. The electron source may further include a magnetic suppressor electrode surrounding at least a portion of the electron emitter. The magnetic suppressor electrode may be formed from one or more magnetic materials. The magnetic suppressor may be configured to shield at least a portion of the electron emitter from an axial magnetic field. The electron source may further include an extractor electrode positioned adjacent to a tip of the electron emitter.

An electron source is disclosed. The electron source may include an electron emitter configured to generate one or more electron beams. The electron source may further include a magnetic suppressor electrode surrounding at least a portion of the electron emitter. The magnetic suppressor electrode may be formed from one or more magnetic materials. The magnetic suppressor may be configured to shield at least a portion of the electron emitter from an axial magnetic field. The electron source may further include an extractor electrode positioned adjacent to a tip of the electron emitter.

An electrostatic beam transfer lens for a multi-beam apparatus that includes a series of multiple, successive electrodes, such that an aperture bore of each electrode is aligned along an electron gun axis and is configured to allow multiple beams to pass therethrough. The first electrode in the series is a cylindrical electrode configured to receive the multiple beams at an entrance plane. The first electrode has a bore length and a bore diameter such that a ratio of bore diameter/bore length<0.3. The shape of the first electrode defines the electrostatic field penetration to the entrance plane of the first electrode to prevent lens focusing fields of the electrostatic beam transfer lens from extending through the first electrode and beyond the entrance plane, thus providing a uniform, flat electric field at the entrance area of the electrostatic transfer lens.

This invention provides a charged particle source, which comprises an emitter and means fo generating a magnetic field distribution. The magnetic field distribution is minimum, about zero, or preferred zero at the tip of the emitter, and along the optical axis is maximum away from the tip immediately. In a preferred embodiment, the magnetic field distribution is provided by dual magnetic lens which provides an anti-symmetric magnetic field at the tip, such that magnetic field at the tip is zero.

This invention provides a charged particle source, which comprises an emitter and means fo generating a magnetic field distribution. The magnetic field distribution is minimum, about zero, or preferred zero at the tip of the emitter, and along the optical axis is maximum away from the tip immediately. In a preferred embodiment, the magnetic field distribution is provided by dual magnetic lens which provides an anti-symmetric magnetic field at the tip, such that magnetic field at the tip is zero.

A charged-particle source for generating a charged-particle comprises a sequence of electrodes, including an emitter electrode with an emitter surface, a counter electrode held at an electrostatic voltage with respect to the emitter electrode at a sign opposite to that of the electrically charged particles, and one or more adjustment electrodes surrounding the source space between the emitter electrode and the counter electrode. These electrodes have a basic overall rotational symmetry along a central axis, with the exception of one or more steering electrodes which is an electrode which interrupts the radial axial-symmetry of the electric potential of the source, for instance tilted or shifted to an eccentric position or orientation, configured to force unintended, secondary charged particles away from the emission surface.

An electron beam system for wafer inspection and review of 3D devices provides a depth of focus up to 20 microns. To inspect and review wafer surfaces or sub-micron-below surface defects with low landing energies in hundreds to thousands of electron Volts, a Wien-filter-free beam splitting optics with three magnetic deflectors can be used with an energy-boosting upper Wehnelt electrode to reduce spherical and chromatic aberration coefficients of the objective lens.

An electron beam system for wafer inspection and review of 3D devices provides a depth of focus up to 20 microns. To inspect and review wafer surfaces or sub-micron-below surface defects with low landing energies in hundreds to thousands of electron Volts, a Wien-filter-free beam splitting optics with three magnetic deflectors can be used with an energy-boosting upper Wehnelt electrode to reduce spherical and chromatic aberration coefficients of the objective lens.