Magnetic lenses, charged particle microscope systems including the same, and associated methods. In an example, a magnetic lens is configured to direct a charged particle beam to a sample location and comprises a plurality of pole pieces and at least two independent coils. The magnetic lens operates as an objective lens with variable main objective plane without immersing a sample in a magnetic field. The variable main objective plane permits selective adjustment of a magnification of the charged particle beam at the focal plane without immersing the sample location in the magnetic fields produced by coils of the magnetic lens. In an example, a charged particle microscope system comprises a charged particle source, a sample holder, and a magnetic objective lens. In an example, a method comprises positioning a sample relative to a magnetic lens and operating the magnetic lens to focus a charged particle beam to a focus location.

A permanently sealed vacuum tube is used to provide the electrons for an electron microscope. This advantageously allows use of low vacuum at the sample, which greatly simplifies the overall design of the system. There are two main variations. In the first variation, imaging is provided by mechanically scanning the sample. In the second variation, imaging is provided by point projection. In both cases, the electron beam is fixed and does not need to be scanned during operation of the microscope. This also greatly simplifies the overall system.

A permanently sealed vacuum tube is used to provide the electrons for an electron microscope. This advantageously allows use of low vacuum at the sample, which greatly simplifies the overall design of the system. There are two main variations. In the first variation, imaging is provided by mechanically scanning the sample. In the second variation, imaging is provided by point projection. In both cases, the electron beam is fixed and does not need to be scanned during operation of the microscope. This also greatly simplifies the overall system.

A particle beam system includes a multi-beam particle source and a magnetic multi-deflector array. The magnetic multi-deflector array includes a coil that is arranged such that, during use of the particle beam system, a multiplicity of individual particle beams substantially passes through the first coil so that they are deflected in an azimuthal direction to correct an azimuthal telecentricity error of the particle beam system so that the individual particle beams telecentrically impinge on an object plane of the particle beam system.

A scanning electron microscope (SEM) with a swing objective lens (SOL) reduces the off-aberrations to enhance the image resolution, and extends the e-beam scanning angle. The scanning electron microscope comprises a charged particle source, an accelerating electrode, and a swing objective lens system including a pre-deflection unit, a swing deflection unit and an objective lens, all of them are rotationally symmetric with respect to an optical axis. The upper inner-face of the swing deflection unit is tilted an angle to the outer of the SEM and its lower inner-face is parallel to the optical axis. A distribution for a first and second focusing field of the swing objective lens is provided to limit the off-aberrations and can be performed by a single swing deflection unit. Preferably, the two focusing fields are overlapped by each other at least 80 percent.

In a transmission electron microscope, an intermediate lens assembly receives a beam of electrons after leaving a primary lens and forms an image of a sample in a sample holder. The intermediate lens assembly comprises a first lens, a second lens, a first port in a first port plane and a second port in a second port plane. The first port and the second port receive a wave front manipulating device for manipulating the wave front of the beam. In a first mode, a controller controls the first and second lenses to direct the diffraction pattern into a second diffraction plane wherein the second diffraction plane is coincident with the first port plane. In a second mode, the controller controls the first and second lenses to direct the diffraction pattern into a third diffraction plane wherein the third diffraction plane is coincident with the second port plane.

Systems and methods of imaging a sample using a charged-particle beam apparatus are disclosed. The apparatus may include a charged-particle source configured to emit charged particles, an aperture plate configured to form a primary charged-particle beam along a primary optical axis from the emitted charged particles, a plurality of primary charged-particle beam deflectors configured to deflect the primary charged-particle beam to be incident on a surface of a sample to define a center of a field-of-view (FOV), and a controller including circuitry configured to apply a first excitation signal to a primary charged-particle beam deflector of the plurality of primary charged-particle beam deflectors to cause the primary charged-particle beam to scan a portion of the FOV of the sample, and apply a second excitation signal to cause the primary-charged particle beam deflector to compensate for an off-axis aberration of the primary charged-particle beam in the portion of the FOV.

Charged-particle detectors using scintillators are situated in a vacuum chamber and include a photomultiplier tube (PMT) that is situated at or near a pole piece of a magnetic objective lens. To maintain satisfactory PMT operation, the PMT is situated within a PMT shield constructed of a high saturation value magnetic material. With the disclosed shields, PMT operation in strong magnetic fields is satisfactory, even for magnetic field magnitudes of at least 0.5 T.

A charged particle lens for focusing a beam of charged particles towards a sample mounted at a sample position. The charged particle lens comprises a first pole piece, a second pole piece, a lens coil and at least one voltage supply. The second pole piece is electrically insulated from the first pole piece and has a central aperture, wherein the second pole piece is arranged to be aligned with the first pole piece, which also has a central aperture, such that a central axis of the charged particle lens extends through the central aperture of the first pole piece and the second pole piece. The lens coil is arranged to generate a magnetic field at the first and second pole pieces, and the at least one voltage supply is arranged to apply a potential difference between the second pole piece and the sample to generate an electric field.

A multiple particle beam system comprises a magnetic immersion lens and a detection system. A cross-over of the second individual particle beams is provided in the secondary path between the beam switch and the detection system, and a contrast aperture with a central cutout for cutting out the secondary beams is arranged in the region of the cross-over. A contrast correction lens system with a first magnetic contrast correction lens is arranged between the objective lens and the contrast aperture. The contrast correction lens system is configured to generate a magnetic field with an adjustable strength and correct beam tilts of the secondary beams in the cross-over in relation to the optical axis of the multiple particle beam system. It is possible to obtain a more uniform contrast for different individual images and the contrast can be improved overall.