Abstract:
An electron source is formed by at least one elementary electron emitter in which an emissive point having a very small radius of curvature operates on the field emission principle and produces an electron beam, the intensity of which is independent of any possible variations of electron emission. The emissive point cooperates with an extracting electrode, and a control electrode having a negative potential with respect to the extracting electrode is placed downstream of the extracting electrode with respect to the direction of propagation of the beam.
Abstract:
A gun configured to generate charged particles, comprising a ring-cathode (200) electrically configured to generate a charged particle beam; a lens arranged to focus the charged particle beam on a specimen; and at least one correction focusing electrode (1406) arranged to generate at least one electrostatic/magnetic field to further divergently/convergently focus the charged particle beam for correcting in-plane geometric aberrations associated with the lens, the focusing being based on the in-plane geometric aberrations associated with the lens. A related method is also disclosed.
Abstract:
An electron beam device including an electron source which generates an electron beam; three lenses for controlling the characteristics of the electron beam, including a first lens, second lens and third lens arranged in sequence from the upstream side in relation to the emission direction of the electron beam; and a beam definition aperture arranged on the second lens. The position of the second lens is adjusted such that the total lens magnification ratio obtained under maximum beam current substantially matches the ideal lens magnification ratio defined on the basis of electro-optical characteristics.
Abstract:
An electrostatic charged particle beam lens includes an electrode including a flat plate having a first surface having a normal line extending in a direction of an optical axis and a second surface opposite to the first surface, the electrode having a through-hole extending from the first surface to the second surface. When an opening cross section is defined as a cross section of the through-hole taken along a plane perpendicular to the normal line and a representative diameter is defined as a diameter of a circle obtained by performing regression analysis of the opening cross section, a representative diameter of the opening cross section in a first region that is on the first surface side and a representative diameter of the opening cross section in a second region that is on the second surface side are each larger than a representative diameter of the opening cross section in a third region that is a region in the electrode disposed between the first surface and the second surface.
Abstract:
A ion source comprises: a chamber (45), an injection to inject matter into the chamber, wherein said matter comprises at least a first species, a tip with an apex located in the chamber, wherein the apex has a surface made of a metallic second species, a generator to generate ions of said species, and a regulation system adapted to set operative conditions of the chamber to alternatively generate ions from the gaseous first species, and ions from the non-gaseous metallic second species.
Abstract:
A charged particle optical system includes: a member 112 likely deforming due to heat; and an electrostatic deflector 113 deflecting a charged particle beam 1 and fixed to the member 112. An electrode supporting portion 5 is placed on the fixing portion 7 so as to reduce a transmission of a deforming stress from the member 112 to the electrode supporting portion 5 in a direction of the electric field through the fixing portion 7. The transmission of the stress from the member that causes deformation to the electrode supporting portion of the electrostatic deflector is suppressed, and the dispersion of the deflections of a plurality of the charged particle beams is reduced.
Abstract:
A charged particle detection system comprises plural detection elements and a multi-aperture plate in proximity of the detection elements. Charged particle beamlets can traverse the apertures of the multi-aperture plate to be incident on the detection elements. More than one multi-aperture plate can be provided to form a stack of multi-aperture plates in proximity of the detector. A suitable electric potential supplied to the multi-aperture plate can have an energy filtering property for the plural charged particle beamlets traversing the apertures of the plate.
Abstract:
A method for milling of a workpiece of inert material by nanodroplet beam sputtering includes the steps of providing aliquid; electrohydrodynamically atomizing the liquid to form charged nanodroplets; and directing the atomized charged nanodroplets onto the workpiece to selectively remove material. The method is used for broad-beam milling the workpiece of inert material, for precision micromachining and/or for three dimensionally profiling organic samples via secondary ion mass spectrometry. The liquid is electrosprayed in a cone-jet mode in a vacuum and average nanodroplet diameter, nanodroplet velocity, and molecular energy of the nanodroplets is adjusted by changing liquid flow rate and the acceleration voltage applied to the ionic liquid as it is atomized. Apparatus for performing the method are also included embodiments.
Abstract:
The present invention relates to an electron lens for use in an microcolumn, and more particularly to a multipole electron lens wherein the electron lens includes two or more electrode layers, each of the electrode layers has a slit aperture extending across a central optical axis along which an electron beam passes, and the two electrode layers are aligned on an electron optical axis such that the slit apertures are staggered with each other. Further, the present invention relates to a microcolumn using the multipole lens. The multipole lens according to the present invention can be manufactured and controlled in a simple fashion, reduces the defocusing of the microcolumn, and increases an active deflection area.
Abstract:
An apparatus for manipulating the trajectories of moving charged particles. The apparatus includes a grid of laterally spaced side by side elongate elements and means defining a path for charged particles to traverse the grid. The grid is supported and configured for application of a voltage gradient between and/or along the elongate elements, whereby to manipulate the trajectories of charged particles that traverse the grid. A method of manipulating the trajectories of moving charged particles is also disclosed.