A multi-beam lens device is described, which includes: a first beam passage for a first charged particle beam formed along a first direction between a first beam inlet of the first beam passage and a first beam outlet of the first beam passage; a second beam passage for a second charged particle beam formed along a second direction between a second beam inlet of the second beam passage and a second beam outlet of the second beam passage, wherein the first direction and the second direction are inclined with respect to each other by an angle () of 5 or more such that the first beam passage approaches the second beam passage toward the first beam outlet; and a common excitation coil or a common electrode arrangement configured for focussing the first charged particle beam and the second charged particle beam. Further, a charged particle beam device as well as a method of operating a multi-beam lens device are described.

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 and apparatus are disclosed for improving resolution and duty-cycle of a multi-reflecting TOF mass spectrometer (MR-TOF) by arranging a cylindrical analyzer having an appropriate radial deflection means, means for limiting ion divergence in the tangential direction and a pulsed source providing ion packet divergence of less than 1 mm*deg. There are disclosed embodiments for fifth-order focusing cylindrical ion minors. Separate embodiments provide parallel tandem MS-MS within a single cylindrical MR-TOF.

A charged-particle microscope having a vacuum chamber comprises a specimen holder, a particle-optical column, a detector and an exchangeable column extending element. The specimen holder is for holding a specimen. The particle-optical column is for producing and directing a beam of charged particles along an axis so as to irradiate the specimen. The column has a terminal pole piece at an extremity facing the specimen holder. The detector is for detecting a flux of radiation emanating from the specimen in response to irradiation by the beam. The exchangeable column extending element is magnetically mounted on the pole piece in a space between the pole piece and the specimen holder. Methods of using the microscope are also disclosed.

This composite charged particle beam device comprises a first charged particle beam column (6), a second charged particle beam column (1) which is equipped with a deceleration system, and is equipped with a detector (3) inside the column, a test piece stage (10) on which a test piece (9) is placed, and an electric field correction electrode (13) which is provided around the tip of the first charged particle beam column, wherein the electric field correction electrode is an electrode that corrects the electric field distribution formed in the vicinity of the test piece, and the electric field correction electrode is positioned between the test piece and the first charged particle beam column, and on the opposite side from the second charged particle beam column with respect to the optical axis of the first charged particle beam column.

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.

An ion beam lens and methods for combining ion beams are disclosed. Embodiments combine hyperthermal ion beams and can include layered three-dimensional electrodes with passageways through the electrodes, each electrode having a specified DC voltage and each passageway configured for passing an ion beam to an exit, the velocity vectors of the beams being primarily oriented along the lens' central axis upon exiting the passageways. Embodiments include nested electrode plates with curved ion beam passageways. In some embodiments each electrode plate has a charge different from the electrode plates adjacent to it, and in some embodiments every other electrode plate is charged with a first DC voltage and the remaining plates are charged with a second DC voltage different from the first DC voltage.

An electrostatic lens for transporting charged particles in an axial direction includes a first group of first electrodes configured to receive a first DC potential from a DC voltage source, and a second group of second electrodes configured to receive a second DC potential from the DC voltage source different from the first DC potential. The first electrodes are interdigitated with the second electrodes. The first group and/or the second group has a geometric feature that progressively varies along the axial direction. The lens generates an axial potential profile that progressively changes along the axial direction, and thereby reduces geometrical aberrations. The lens may be part of a charged particle processing apparatus such as, for example, a mass spectrometer or an electron microscope.